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  <title>[HST REPORTS]</title>
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  <updated>2010-08-01T00:58:29Z</updated>
  <author>
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  <entry>
    <title>Daily Report #5149</title>
    <link rel="alternate" href="http://www.aus-city.com/cgi-bin/dada/mail.cgi/archive/HST_REPORTS/20100731020504/"/>
    <id>tag:www.aus-city.com,2010-07-31:%2Fcgi-bin%2Fdada%2Fmail.cgi%2Farchive%2FHST_REPORTS%2F20100731020504%2F</id>
    
    <published>2010-07-31T02:05:04Z</published>
    <updated>2010-07-31T02:05:04Z</updated>
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&lt;div class=WordSection1&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;HUBBLE
SPACE TELESCOPE - Continuing to Collect World Class Science &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;DAILY
REPORT #5149 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;PERIOD
COVERED: 5am July 29 - 5am July 30, 2010 (DOY 210/09:00z-211/09:00z) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;FLIGHT
OPERATIONS SUMMARY: &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Significant
Spacecraft Anomalies: (The following are preliminary reports&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;of
potential non-nominal performance that will be investigated.) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;HSTARS:
(None) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COMPLETED
OPS REQUEST: (None) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COMPLETED
OPS NOTES: (None) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;SCHEDULED SUCCESSFUL&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;FGS
GSAcq &amp;#160;&amp;#160;
&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;9
&amp;#160;&amp;#160;&amp;#160;&amp;#160; &amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;9 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;FGS
REAcq &amp;#160;&amp;#160;
&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;6
&amp;#160;&amp;#160;&amp;#160;&amp;#160; &amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;6 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;OBAD
with Maneuver 6 &amp;#160;&amp;#160;&amp;#160;&amp;#160;
&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;6 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;SIGNIFICANT
EVENTS: (None) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;OBSERVATIONS
SCHEDULED: &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;ACS/WFC3
11593 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Dynamical
Masses of the Coolest Brown Dwarfs &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;T
dwarfs are excellent laboratories to study the evolution and the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;atmospheric
physics of both brown dwarfs and extrasolar planets. To&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;date,
only a single T dwarf binary has a dynamical mass determination,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;and
more are sorely needed. The prospects of measuring more dynamical&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;masses
over the next decade are limited to 6 known short-period T dwarf&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;binaries.
We propose here to obtain Long-Term HST/ACS monitoring for the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;3
of the 6 binaries which cannot be resolved with AO from the ground.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Upon
completion, our program will substantially increase the number of T&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;dwarf
dynamical mass measurements and thereby provide key benchmarks for&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;testing
theoretical models of ultracool objects. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COS/NUV/FUV
12086 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Generation
of 1-D Fixed Pattern Templates &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Tests
have shown that application of a 1-D fixed pattern template to a&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COS
spectrum can reduce the fixed pattern noise in G130M or G160M&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;spectra
to an equivalent S/N of about 30/1. For this to be occur, the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;template
must be derived from data for the same grating and nearly the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;same
central wavelength as the observation. This is because each grating&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;has
a different cross dispersion profile, and different central&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;wavelengths
fall at different cross dispersion detector locations. As a&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;result,
spectra obtained at each grating and central wavelength setting&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;are
derived from different regions of the detectors -- each with their&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;own,
unique detector features and grid wire shadows. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;STIS/CC
11845 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;CCD
Dark Monitor Part 2 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Monitor
the darks for the STIS CCD. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;STIS/CC
11847 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;CCD
Bias Monitor-Part 2 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Monitor
the bias in the 1x1, 1x2, 2x1, and 2x2 bin settings at gain=1,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;and
1x1 at gain = 4, to build up high-S/N superbiases and track the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;evolution
of hot columns. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;STS/MA/CC
12085 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;STIS/E230M
Observations of HD6655 for Calibration of COS/G230L &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;This
program observes HD 6655, a radial velocity target that is used for&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;calibrating
COS/G230L. The objective of this program is to get STIS data&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;of
this target, with the E230M grating, and then use this observations&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;to
derive the offsets between the internal and external COS/G230L&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;wavelength
scales. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/ACS/IR
11677 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Is
47 Tuc Young? Measuring its White Dwarf Cooling Age and Completing a&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Hubble
Legacy &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;With
this proposal we will firmly establish the age of 47 Tuc from its&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;cooling
white dwarfs. 47 Tuc is the nearest and least reddened of the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;metal-rich
disk globular clusters. It is also the template used for&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;studying
the giant branches of nearby resolved galaxies. In addition,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the
age sensitive magnitude spread between the main sequence turnoff and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;horizontal
branch is identical for 47 Tuc, two bulge globular clusters&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;and
the bulge field population. A precise relative age constraint for 47&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Tuc,
compared to the halo clusters M4 and NGC 6397, both of which we&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;recently
dated via white dwarf cooling, would therefore constrain when&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the
bulge formed relative to the old halo globular clusters. Of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;particular
interest is that with the higher quality ACS data on NGC&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;6397,
we are now capable with the technique of white dwarf cooling of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;determining
ages to an accuracy of +/-0.4 Gyrs at the 95% confidence&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;level.
Ages derived from the cluster turnoff are not currently capable&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;of
reaching this precision. The important role that 47 Tuc plays in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;galaxy
formation studies, and as the metal-rich template for the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;globular
clusters, makes the case for a white dwarf cooling age for this&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;metal-rich
cluster compelling. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Several
recent analyses have suggested that 47 Tuc is more than 2 Gyrs&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;younger
than the Galactic halo. Others have suggested an age similar to&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;that
of the most metal poor globular clusters. The current situation is&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;clearly
uncertain and obviously a new approach to age dating this&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;important
cluster is required. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;With
the observations of 47 Tuc, this project will complete a legacy for&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;HST.
It will be the third globular cluster observed for white dwarf&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;cooling;
the three covering almost the full metallicity range of the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;cluster
system. Unless JWST has its proposed bluer filters (700 and 900&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;nm)
this science will not be possible perhaps for decades until a large&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;optical
telescope is again in space. Ages for globular clusters from the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;main
sequence turnoff are less precise than those from white dwarf&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;cooling
making the science with the current proposal truly urgent. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/IR/S/C
11929 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;IR
Dark Current Monitor &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Analyses
of ground test data showed that dark current signals are more&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;reliably
removed from science data using darks taken with the same&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;exposure
sequences as the science data, than with a single dark current&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;image
scaled by desired exposure time. Therefore, dark current images&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;must
be collected using all sample sequences that will be used in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;science
observations. These observations will be used to monitor changes&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;in
the dark current of the WFC3-IR channel on a day-to-day basis, and to&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;build
calibration dark current ramps for each of the sample sequences to&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;be
used by Gos in Cycle 17. For each sample sequence/array size&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;combination,
a median ramp will be created and delivered to the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;calibration
database system (CDBS). &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UV
11554 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Luminosity
Profiles of Extremely Massive Clusters in NGC 7252 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;The
galactic merger remnant NGC 7252 represents one of the most extreme&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;post-starburst
environments in the local universe. During the disk-disk&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;merger
(~400 Myr ago) this galaxy produced the largest young massive&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;star
cluster population known, including two clusters above 10^7 Msun, a&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;factor
of 100 more massive than typical globular clusters in the Milky&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Way.
We propose ACS-HRC observations of 3 fields in NGC 7252 in order to&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;explore
the detailed properties, i.e. luminosity profiles, of these&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;massive
star clusters. These observations will be able to test massive&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;cluster
formation mechanisms (e.g. the cluster merger scenario) as well&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;as
the possible tidal erosion and truncation of the outer regions of the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;clusters
by the galactic tidal field. These observations will compliment&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;our
large on-going study using archival HST data, of star cluster&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;profiles
outside the Local Group. The cluster population in NGC 7252&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;will
extend our sample in cluster mass by an order of magnitude. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UVIS
11905 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3
UVIS CCD Daily Monitor &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;The
behavior of the WFC3 UVIS CCD will be monitored daily with a set of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;full-frame,
four-amp bias and dark frames. A smaller set of 2Kx4K&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;subarray
biases are acquired at less frequent intervals throughout the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;cycle
to support subarray science observations. The internals from this&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;proposal,
along with those from the anneal procedure (Proposal 11909),&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;will
be used to generate the necessary superbias and superdark reference&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;files
for the calibration pipeline (CDBS). &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UVIS
11908 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Cycle
17: UVIS Bowtie Monitor &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Ground
testing revealed an intermittent hysteresis type effect in the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;UVIS
detector (both CCDs) at the level of ~1%, lasting hours to days.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Initially
found via an unexpected bowtie-shaped feature in flatfield&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;ratios,
subsequent lab tests on similar e2v devices have since shown&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;that
it is also present as simply an overall offset across the entire&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;CCD,
i.e., a QE offset without any discernable pattern. These lab tests&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;have
further revealed that overexposing the detector to count levels&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;several
times full well fills the traps and effectively neutralizes the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;bowtie.
Each visit in this proposal acquires a set of three 3x3 binned&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;internal
flatfields: the first unsaturated image will be used to detect&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;any
bowtie, the second, highly exposed image will neutralize the bowtie&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;if
it is present, and the final image will allow for verification that&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the
bowtie is gone. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UVIS/IR
11644 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;A
Dynamical-Compositional Survey of the Kuiper Belt: A New Window Into&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the
Formation of the Outer Solar System &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;The
eight planets overwhelmingly dominate the solar system by mass, but&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;their
small numbers, coupled with their stochastic pasts, make it&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;impossible
to construct a unique formation history from the dynamical or&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;compositional
characteristics of them alone. In contrast, the huge&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;numbers
of small bodies scattered throughout and even beyond the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;planets,
while insignificant by mass, provide an almost unlimited number&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;of
probes of the statistical conditions, history, and interactions in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the
solar system. To date, attempts to understand the formation and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;evolution
of the Kuiper Belt have largely been dynamical simulations&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;where
a hypothesized starting condition is evolved under the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;gravitational
influence of the early giant planets and an attempt is&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;made
to reproduce the current observed populations. With little&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;compositional
information known for the real Kuiper Belt, the test&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;particles
in the simulation are free to have any formation location and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;history
as long as they end at the correct point. Allowing compositional&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;information
to guide and constrain the formation, thermal, and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;collisional
histories of these objects would add an entire new dimension&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;to
our understanding of the evolution of the outer solar system. While&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;ground
based compositional studies have hit their flux limits already&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;with
only a few objects sampled, we propose to exploit the new&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;capabilities
of WFC3 to perform the first ever large-scale&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;dynamical-compositional
study of Kuiper Belt Objects (KBOs) and their&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;progeny
to study the chemical, dynamical, and collisional history of the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;region
of the giant planets. The sensitivity of the WFC3 observations&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;will
allow us to go up to two magnitudes deeper than our ground based&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;studies,
allowing us the capability of optimally selecting a target list&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;for
a large survey rather than simply taking the few objects that can be&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;measured,
as we have had to do to date. We have carefully constructed a&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;sample
of 120 objects which provides both overall breadth, for a general&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;understanding
of these objects, plus a large enough number of objects in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the
individual dynamical subclass to allow detailed comparison between&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;and
within these groups. These objects will likely define the core&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Kuiper
Belt compositional sample for years to come. While we have many&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;specific
results anticipated to come from this survey, as with any&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;project
where the field is rich, our current knowledge level is low, and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;a
new instrument suddenly appears which can exploit vastly larger&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;segments
of the population, the potential for discovery -- both&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;anticipated
and not -- is extraordinary.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

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  <entry>
    <title>Daily Report #5147</title>
    <link rel="alternate" href="http://www.aus-city.com/cgi-bin/dada/mail.cgi/archive/HST_REPORTS/20100729020504/"/>
    <id>tag:www.aus-city.com,2010-07-29:%2Fcgi-bin%2Fdada%2Fmail.cgi%2Farchive%2FHST_REPORTS%2F20100729020504%2F</id>
    
    <published>2010-07-29T02:05:04Z</published>
    <updated>2010-07-29T02:05:04Z</updated>
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&lt;div class=WordSection1&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;HUBBLE
SPACE TELESCOPE - Continuing to Collect World Class Science &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;DAILY
REPORT #5147 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;PERIOD
COVERED: 5am July 27 - 5am July 28, 2010 (DOY 208/09:00z-209/09:00z) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;FLIGHT
OPERATIONS SUMMARY: &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Significant
Spacecraft Anomalies: (The following are preliminary reports&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;of
potential non-nominal performance that will be investigated.) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;HSTARS:&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;12342
- REAcq(2,1,1) at 209/06:54:02z resulted in a &amp;#34;scan step limit
exceeded&amp;#34;&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&amp;#160;&amp;#160; error in FGS2 on the first attempt. The REAcq went on to succeed
on the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&amp;#160;&amp;#160; second attempt. &amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160; &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&amp;#160;&amp;#160; Observations possibly affected WFC 73-75, Proposal ID#11700; COS
45,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&amp;#160;&amp;#160; Proposal ID#11598 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COMPLETED
OPS REQUEST: (None) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COMPLETED
OPS NOTES: (None) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;SCHEDULED SUCCESSFUL&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;FGS
GSAcq &amp;#160;&amp;#160; &amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;7
&amp;#160;&amp;#160;&amp;#160;&amp;#160; &amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;7
&amp;#160;&amp;#160;&amp;#160; &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;FGS
REAcq &amp;#160;&amp;#160;
&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;8
&amp;#160;&amp;#160;&amp;#160;&amp;#160; &amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;8 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;OBAD
with Maneuver 4 &amp;#160;&amp;#160;&amp;#160;&amp;#160;
&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;4 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;SIGNIFICANT
EVENTS: (None) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;OBSERVATIONS
SCHEDULED: &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COS/NUV/FUV
11598 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;How
Galaxies Acquire their Gas: A Map of Multiphase Accretion and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Feedback
in Gaseous Galaxy Halos &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;We
propose to address two of the biggest open questions in galaxy&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;formation
- how galaxies acquire their gas and how they return it to the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;IGM
- with a concentrated COS survey of diffuse multiphase gas in the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;halos
of SDSS galaxies at z = 0.15 - 0.35. Our chief science goal is to&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;establish
a basic set of observational facts about the physical state,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;metallicity,
and kinematics of halo gas, including the sky covering&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;fraction
of hot and cold material, the metallicity of infall and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;outflow,
and correlations with galaxy stellar mass, type, and color -&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;all
as a function of impact parameter from 10 - 150 kpc. Theory suggests&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;that
the bimodality of galaxy colors, the shape of the luminosity&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;function,
and the mass-metallicity relation are all influenced at a&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;fundamental
level by accretion and feedback, yet these gas processes are&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;poorly
understood and cannot be predicted robustly from first&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;principles.
We lack even a basic observational assessment of the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;multiphase
gaseous content of galaxy halos on 100 kpc scales, and we do&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;not
know how these processes vary with galaxy properties. This ignorance&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;is
presently one of the key impediments to understanding galaxy&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;formation
in general. We propose to use the high-resolution gratings&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;G130M
and G160M on the Cosmic Origins Spectrograph to obtain sensitive&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;column
density measurements of a comprehensive suite of multiphase ions&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;in
the spectra of 43 z &amp;#60; 1 QSOs lying behind 43 galaxies selected from&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the
Sloan Digital Sky Survey. In aggregate, these sightlines will&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;constitute
a statistically sound map of the physical state and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;metallicity
of gaseous halos, and subsets of the data with cuts on&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;galaxy
mass, color, and SFR will seek out predicted variations of gas&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;properties
with galaxy properties. Our interpretation of these data will&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;be
aided by state-of-the-art hydrodynamic simulations of accretion and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;feedback,
in turn providing information to refine and test such models.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;We
will also use Keck, MMT, and Magellan (as needed) to obtain optical&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;spectra
of the QSOs to measure cold gas with Mg II, and optical spectra&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;of
the galaxies to measure SFRs and to look for outflows. In addition to&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;our
other science goals, these observations will help place the Milky&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Way's
population of multiphase, accreting High Velocity Clouds (HVCs)&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;into
a global context by identifying analogous structures around other&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;galaxies.
Our program is designed to make optimal use of the unique&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;capabilities
of COS to address our science goals and also generate a&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;rich
dataset of other absorption-line systems. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;ACS/WFC3
11670 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;The
Host Environments of Type Ia Supernovae in the SDSS Survey &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;The
Sloan Digital Sky Survey Supernova Survey has discovered nearly 500&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;type
Ia supernovae and created a large, unique, and uniform sample of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;these
cosmological tools. As part of a comprehensive study of the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;supernova
hosts, we propose to obtain Hubble ACS images of a large&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;fraction
of these galaxies. Integrated colors and spectra will be&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;measured
from the ground, but we require high-resolution HST imaging to&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;provide
accurate morphologies and color information at the site of the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;explosion.
This information is essential in determining the systematic&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;effects
of population age on type Ia supernova luminosities and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;improving
their reliability in measuring dark energy. Recent studies&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;suggest
two populations of type Ia supernovae: a class that explodes&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;promptly
after star-formation and one that is delayed by billions of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;years.
Measuring the star-formation rate at the site of the supernova&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;from
colors in the HST images may be the best way to differentiate&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;between
these classes. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COS/NUV/S/C/FUV
12082 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Extending
COS/G130M Coverage Down to 905A With Two New Central&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Wavelengths.
&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;These
exploratory observations will provide sensitivity, wavelength&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;range,
and resolution measurements for two new COS FUV G130M central&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;wavelength
settings. These new settings will extend COS/G130M coverage&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;down
to 905? in two new bandpasses; 1021-1171? (BLUE) and 905-1055?&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;(Ultra-BLUE).
The modes are chosen to provide continuous coverage from&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;905?
to the existing coverage in the G130M/1291? setting with&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;approximately
30? of overlap in each mode for cross-calibration&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;purposes.
No focus adjustments will be made for these settings, as this&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;is
deemed an unnecessary risk to COS. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;These
new modes have the potential to provide greater than FUSE&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;sensitivity
at moderate (3, 000-5, 000) resolution. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Three
WD targets are defined; &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;1)
GD50 (GSC-04717-00588; a well observed standard WD) 2) WD0320-539&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;(GSC-08493-00891,
one of the targets used in exploring the G140L&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;sensitivity),
3) REJ0503-289 (WD-5001-289 = GSC-04717-00588, a hot EUVE&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;bright
WD) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;But
only target 2) is used at this time. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;In
the observations section, G130M/1291A is a placeholder for the BLUE&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;and
Super-BLUE settings. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;STIS/CC
11845 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;CCD
Dark Monitor Part 2 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Monitor
the darks for the STIS CCD. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;STIS/CC
11847 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;CCD
Bias Monitor-Part 2 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Monitor
the bias in the 1x1, 1x2, 2x1, and 2x2 bin settings at gain=1,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;and
1x1 at gain = 4, to build up high-S/N superbiases and track the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;evolution
of hot columns. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/IR
11933 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;IR
Rate Dependent Non-linearity &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;The
NICMOS non-linearity known as the Bohlin Effect has revealed that&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the
apparent flux of a source observed by NICMOS is not a simple, linear&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;function
of count rate. The effect has been characterized by&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;observations
of star clusters observed with and without additional&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;background
from the internal lamps. As WFC3 lacks internal lamps which&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;can
be used to add background, we will rely on the bright Earth limb to&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;provide
additional background. We will observe a star cluster, 47 Tuc,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;repeatedly
throughout a complete HST orbit which has been chosen to put&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the
closest approach to the bright Earth to be 13.5 degrees, the closest&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;approach
allowed while retaining FGS guiding. Another set will be done&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;with
the BE limb closest approach of 15.5 degrees. The observations will&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;be
done with the two most commonly used filters, F110W and F160W and at&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;two
different bright Earth limb angles to test the linearity of the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;non-linearity.
We have also included an orbit on NGC 1850 to repeat the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;NICMOS
field for which the linearity of the field has been established. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/IR/S/C
11929 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;IR
Dark Current Monitor &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Analyses
of ground test data showed that dark current signals are more&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;reliably
removed from science data using darks taken with the same&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;exposure
sequences as the science data, than with a single dark current&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;image
scaled by desired exposure time. Therefore, dark current images&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;must
be collected using all sample sequences that will be used in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;science
observations. These observations will be used to monitor changes&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;in
the dark current of the WFC3-IR channel on a day-to-day basis, and to&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;build
calibration dark current ramps for each of the sample sequences to&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;be
used by Gos in Cycle 17. For each sample sequence/array size&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;combination,
a median ramp will be created and delivered to the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;calibration
database system (CDBS). &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UV/ACS/WFC/IR
12055 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;A
Panchromatic Hubble Andromeda Treasury - I &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;We
propose to image the north east quadrant of M31 to deep limits in the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;UV,
optical, and near-IR. HST imaging should resolve the galaxy into&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;more
than 100 million stars, all with common distances and foreground&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;extinctions.
UV through NIR stellar photometry (F275W, F336W with&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UVIS,
F475W and F814W with ACS/WFC, and F110W and F160W with&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/NIR)
will provide effective temperatures for a wide range of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;spectral
types, while simultaneously mapping M31's extinction. Our&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;central
science drivers are to: understand high-mass variations in the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;stellar
IMF as a function of SFR intensity and metallicity; capture the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;spatially-resolved
star formation history of M31; study a vast sample of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;stellar
clusters with a range of ages and metallicities. These are&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;central
to understanding stellar evolution and clustered star formation;&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;constraining
ISM energetics; and understanding the counterparts and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;environments
of transient objects (novae, SNe, variable stars, x-ray&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;sources,
etc.). As its legacy, this survey adds M31 to the Milky Way and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Magellanic
Clouds as a fundamental calibrator of stellar evolution and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;star-formation
processes for understanding the stellar populations of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;distant
galaxies. Effective exposure times are 977s in F275W, 1368s in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;F336W,
4040s in F475W, 4042s in F814W, 699s in F110W, and 1796s in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;F160W,
including short exposures to avoid saturation of bright sources.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;These
depths will produce photon-limited images in the UV. Images will&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;be
crowding-limited in the optical and NIR, but will reach below the red&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;clump
at all radii. The images will reach the Nyquist sampling limit in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;F160W,
F475W, and F814W. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UVIS
11905 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3
UVIS CCD Daily Monitor &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;The
behavior of the WFC3 UVIS CCD will be monitored daily with a set of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;full-frame,
four-amp bias and dark frames. A smaller set of 2Kx4K&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;subarray
biases are acquired at less frequent intervals throughout the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;cycle
to support subarray science observations. The internals from this&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;proposal,
along with those from the anneal procedure (Proposal 11909),&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;will
be used to generate the necessary superbias and superdark reference&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;files
for the calibration pipeline (CDBS). &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UVIS/IR
11700 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Bright
Galaxies at z&amp;#62;7.5 with a WFC3 Pure Parallel Survey &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;The
epoch of reionization represents a special moment in the history of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the
Universe as it is during this era that the first galaxies and star&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;clusters
are formed. Reionization also profoundly affects the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;environment
where subsequent generations of galaxies evolve. Our&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;overarching
goal is to test the hypothesis that galaxies are responsible&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;for
reionizing neutral hydrogen. To do so we propose to carry out a pure&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;parallel
WFC3 survey to constrain the bright end of the redshift z&amp;#62;7.5&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;galaxy
luminosity function on a total area of 176 arcmin^2 of sky.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Extrapolating
the evolution of the luminosity function from z~6, we&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;expect
to detect about 20 Lyman Break Galaxies brighter than M_* at z~8&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;significantly
improving the current sample of only a few galaxies known&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;at
these redshifts. Finding significantly fewer objects than predicted&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;on
the basis of extrapolation from z=6 would set strong limits to the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;brightness
of M_*, highlighting a fast evolution of the luminosity&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;function
with the possible implication that galaxies alone cannot&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;reionize
the Universe. Our observations will find the best candidates&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;for
spectroscopic confirmation, that is bright z&amp;#62;7.5 objects, which&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;would
be missed by small area deeper surveys. The random pointing nature&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;of
the program is ideal to beat cosmic variance, especially severe for&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;luminous
massive galaxies, which are strongly clustered. In fact our&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;survey
geometry of 38 independent fields will constrain the luminosity&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;function
like a contiguous single field survey with two times more area&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;at
the same depth. Lyman Break Galaxies at z&amp;#62;7.5 down to m_AB=26.85 (5&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;sigma)
in F125W will be selected as F098M dropouts, using three to five&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;orbits
visits that include a total of four filters (F606W, F098M, F125W,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;F160W)
optimized to remove low-redshift interlopers and cool stars. Our&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;data
will be highly complementary to a deep field search for high- z&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;galaxies
aimed at probing the faint end of the luminosity function,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;allowing
us to disentangle the degeneracy between faint end slope and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;M_*
in a Schechter function fit of the luminosity function. We waive&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;proprietary
rights for the data. In addition, we commit to release the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;coordinates
and properties of our z&amp;#62;7.5 candidates within one month from&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the
acquisition of each field. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

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  <entry>
    <title>Daily Report #5146</title>
    <link rel="alternate" href="http://www.aus-city.com/cgi-bin/dada/mail.cgi/archive/HST_REPORTS/20100727230503/"/>
    <id>tag:www.aus-city.com,2010-07-27:%2Fcgi-bin%2Fdada%2Fmail.cgi%2Farchive%2FHST_REPORTS%2F20100727230503%2F</id>
    
    <published>2010-07-27T23:05:03Z</published>
    <updated>2010-07-27T23:05:03Z</updated>
    <content type="html">

&lt;div class=WordSection1&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;HUBBLE
SPACE TELESCOPE - Continuing to Collect World Class Science &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;DAILY
REPORT #5146 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;PERIOD
COVERED: 5am July 26 - 5am July 27, 2010 (DOY 207/09:00z-208/09:00z) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;FLIGHT
OPERATIONS SUMMARY: &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Significant
Spacecraft Anomalies: (The following are preliminary reports&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;of
potential non-nominal performance that will be investigated.) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;HSTARS:
(None) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COMPLETED
OPS REQUEST: (None) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COMPLETED
OPS NOTES: (None) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;SCHEDULED SUCCESSFUL&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;FGS
GSAcq &amp;#160;&amp;#160;
&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;8
&amp;#160;&amp;#160;&amp;#160; &amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;8&amp;#160;
&amp;#160;&amp;#160;&amp;#160; &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;FGS
REAcq &amp;#160;&amp;#160;
&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;9
&amp;#160;&amp;#160;&amp;#160; &amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;9&amp;#160; &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;OBAD
with Maneuver 5 &amp;#160;&amp;#160;&amp;#160;
&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;5&amp;#160; &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;SIGNIFICANT
EVENTS: (None) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;OBSERVATIONS
SCHEDULED: &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;ACS/WFC
11996 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;CCD
Daily Monitor (Part 3) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;This
program comprises basic tests for measuring the read noise and dark&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;current
of the ACS WFC and for tracking the growth of hot pixels. The&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;recorded
frames are used to create bias and dark reference images for&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;science
data reduction and calibration. This program will be executed&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;four
days per week (Mon, Wed, Fri, Sun) for the duration of Cycle 17. To&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;facilitate
scheduling, this program is split into three proposals. This&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;proposal
covers 308 orbits (19.25 weeks) from 21 June 2010 to 1 November&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;2010.
&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COS/FUV
11895 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;FUV
Detector Dark Monitor &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Monitor
the FUV detector dark rate by taking long science exposures&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;without
illuminating the detector. The detector dark rate and spatial&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;distribution
of counts will be compared to pre-launch and SMOV data in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;order
to verify the nominal operation of the detector. Variations of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;count
rate as a function of orbital position will be analyzed to find&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;dependence
of dark rate on proximity to the SAA. Dependence of dark rate&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;as
function of time will also be tracked. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COS/FUV/STIS/CCD/MA1
11592 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Testing
the Origin(s) of the Highly Ionized High-Velocity Clouds: A&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Survey
of Galactic Halo Stars at z&amp;#62;3 kpc &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Cosmological
simulation predicts that highly ionized gas plays an&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;important
role in the formation and evolution of galaxies and their&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;interplay
with the intergalactic medium. The NASA HST and FUSE missions&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;have
revealed high-velocity CIV and OVI absorption along extragalactic&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;sightlines
through the Galactic halo. These highly ionized high-velocity&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;clouds
(HVCs) could cover 85% of the sky and have a detection rate&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;higher
than the HI HVCs. Two competing, equally exciting, theories may&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;explain
the origin of these highly ionized HVCs: 1) the &amp;#34;Galactic&amp;#34;&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;theory,
where the HVCs are the result of feedback processes and trace&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the
disk-halo mass exchange, perhaps including the accretion of matter&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;condensing
from an extended corona; 2) the &amp;#34;Local Group&amp;#34; theory, where&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;they
are part of the local warm-hot intergalactic medium, representing&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;some
of the missing baryonic matter of the Universe. Only direct&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;distance
determinations can discriminate between these models. Our group&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;has
found that some of these highly ionized HVCs have a Galactic origin,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;based
on STIS observations of one star at z&amp;#60;5.3 kpc. We propose an HST&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;FUV
spectral survey to search for and characterize the high velocity NV,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;CIV,
and SiIV interstellar absorption toward 24 stars at much larger&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;distances
than any previous searches (4&amp;#60;d&amp;#60;21 kpc, 3&amp;#60;|z|&amp;#60;13 kpc). COS&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;will
provide atomic to highly ionized species (e.g.,OI, CII, CIV, SiIV)&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;that
can be observed at sufficient resolution (R~22, 000) to not only&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;detect
these highly ionized HVCs but also to model their properties and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;understand
their physics and origins. This survey is only possible&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;because
of the high sensitivity of COS in the FUV spectral range. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COS/NUV
11894 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;NUV
Detector Dark Monitor &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;The
purpose of this proposal is to measure the NUV detector dark rate by&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;taking
long science exposures with no light on the detector. The&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;detector
dark rate and spatial distribution of counts will be compared&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;to
pre-launch and SMOV data in order to verify the nominal operation of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the
detector. Variations of count rate as a function of orbital position&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;will
be analyzed to find dependence of dark rate on proximity to the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;SAA.
Dependence of dark rate as function of time will also be tracked. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COS/NUV
11896 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;NUV
Spectroscopic Sensitivity Monitoring &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;The
purpose of this proposal is to monitor sensitivity of each NUV&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;grating
mode to detect any changes due to contamination or other causes.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;STIS/CC
11845 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;CCD
Dark Monitor Part 2 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Monitor
the darks for the STIS CCD. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;STIS/CC
11847 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;CCD
Bias Monitor-Part 2 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Monitor
the bias in the 1x1, 1x2, 2x1, and 2x2 bin settings at gain=1,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;and
1x1 at gain = 4, to build up high-S/N superbiases and track the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;evolution
of hot columns. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;STIS/CCD
11721 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Verifying
the Utility of Type Ia Supernovae as Cosmological Probes:&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Evolution
and Dispersion in the Ultraviolet Spectra &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;The
study of distant type Ia supernova (SNe Ia) offers the most&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;practical
and immediate discriminator between popular models of dark&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;energy.
Yet fundamental questions remain over possible&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;redshift-dependent
trends in their observed and intrinsic properties.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;High-quality
Keck spectroscopy of a representative sample of 36&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;intermediate
redshift SNe Ia has revealed a surprising, and unexplained,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;diversity
in their rest-frame UV fluxes. One possible explanation is&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;hitherto
undiscovered variations in the progenitor metallicity.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Unfortunately,
this result cannot be compared to local UV data as only&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;two
representative SNe Ia have been studied near maximum light. Taking&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;advantage
of two new `rolling searches' and the restoration of STIS, we&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;propose
a non-disruptive TOO campaign to create an equivalent comparison&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;local
sample. This will allow us to address possible evolution in the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;mean
UV spectrum and its diversity, an essential precursor to the study&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;of
SNe beyond z~1. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;STIS/CCD
11852 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;STIS
CCD Spectroscopic Flats C17 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;The
purpose of this proposal is to obtain pixel-to-pixel lamp flat&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;fields
for the STIS CCD in spectroscopic mode. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UV/ACS/WFC/IR
12055 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;A
Panchromatic Hubble Andromeda Treasury - I &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;We
propose to image the north east quadrant of M31 to deep limits in the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;UV,
optical, and near-IR. HST imaging should resolve the galaxy into&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;more
than 100 million stars, all with common distances and foreground&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;extinctions.
UV through NIR stellar photometry (F275W, F336W with&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UVIS,
F475W and F814W with ACS/WFC, and F110W and F160W with&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/NIR)
will provide effective temperatures for a wide range of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;spectral
types, while simultaneously mapping M31's extinction. Our&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;central
science drivers are to: understand high-mass variations in the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;stellar
IMF as a function of SFR intensity and metallicity; capture the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;spatially-resolved
star formation history of M31; study a vast sample of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;stellar
clusters with a range of ages and metallicities. These are&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;central
to understanding stellar evolution and clustered star formation;&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;constraining
ISM energetics; and understanding the counterparts and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;environments
of transient objects (novae, SNe, variable stars, x-ray&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;sources,
etc.). As its legacy, this survey adds M31 to the Milky Way and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Magellanic
Clouds as a fundamental calibrator of stellar evolution and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;star-formation
processes for understanding the stellar populations of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;distant
galaxies. Effective exposure times are 977s in F275W, 1368s in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;F336W,
4040s in F475W, 4042s in F814W, 699s in F110W, and 1796s in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;F160W,
including short exposures to avoid saturation of bright sources.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;These
depths will produce photon-limited images in the UV. Images will&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;be
crowding-limited in the optical and NIR, but will reach below the red&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;clump
at all radii. The images will reach the Nyquist sampling limit in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;F160W,
F475W, and F814W. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UVIS
11707 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Detecting
Isolated Black Holes through Astrometric Microlensing &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;This
proposal aims to make the first detection of isolated stellar-mass&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;black
holes (BHs) in the Milky Way, and to determine their masses. Until&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;now,
the only directly measured BH masses have come from radial-velocity&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;measurements
of X-ray binaries. Our proposed method uses the astrometric&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;shifts
that occur when a galactic-bulge microlensing event is caused by&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;a
BH lens. Out of the hundreds of bulge microlensing events found&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;annually
by the OGLE and MOA surveys, a few are found to have very long&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;durations
(&amp;#62;200 days). It is generally believed that the majority of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;these
long-duration events are caused by lenses that are isolated BHs. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;To
test this hypothesis, we will carry out high-precision astrometry of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;5
long-duration events, using the ACS/HRC camera. The expected&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;astrometric
signal from a BH lens is &amp;#62;1.4 mas, at least 7 times the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;demonstrated
astrometric precision attainable with the HRC. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;This
proposal will thus potentially lead to the first unambiguous&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;detection
of isolated stellar-mass BHs, and the first direct mass&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;measurement
for isolated stellar-mass BHs through any technique.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Detection
of several BHs will provide information on the frequency of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;BHs
in the galaxy, with implications for the slope of the IMF at high&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;masses,
the minimum mass of progenitors that produce BHs, and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;constraints
on theoretical models of BH formation. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UVIS
11903 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;UVIS
Photometric Zero Points &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;This
proposal obtains the photometric zero points in 53 of the 62&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;UVIS/WFC3
filters: the 18 broad-band filters, 8 medium-band filters, 16&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;narrow-band
filters, and 11 of the 20 quad filters (those being used in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;cycle
17). The observations will be primary obtained by observing the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;hot
DA white dwarf standards GD153 and G191-B2B. A redder secondary&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;standard,
P330E, will be observed in a subset of the filters to provide&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;color
corrections. Repeat observations in 16 of the most widely used&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;cycle
17 filters will be obtained once per month for the first three&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;months,
and then once every second month for the duration of cycle 17,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;alternating
and depending on target availability. These observations&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;will
enable monitoring of the stability of the photometric system.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Photometric
transformation equations will be calculated by comparing the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;photometry
of stars in two globular clusters, 47 Tuc and NGC 2419, to&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;previous
measurements with other telescopes/instruments. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UVIS
11905 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3
UVIS CCD Daily Monitor &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;The
behavior of the WFC3 UVIS CCD will be monitored daily with a set of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;full-frame,
four-amp bias and dark frames. A smaller set of 2Kx4K&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;subarray
biases are acquired at less frequent intervals throughout the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;cycle
to support subarray science observations. The internals from this&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;proposal,
along with those from the anneal procedure (Proposal 11909),&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;will
be used to generate the necessary superbias and superdark reference&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;files
for the calibration pipeline (CDBS).&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-size:12.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

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  <entry>
    <title>Daily Report #5144</title>
    <link rel="alternate" href="http://www.aus-city.com/cgi-bin/dada/mail.cgi/archive/HST_REPORTS/20100724070504/"/>
    <id>tag:www.aus-city.com,2010-07-24:%2Fcgi-bin%2Fdada%2Fmail.cgi%2Farchive%2FHST_REPORTS%2F20100724070504%2F</id>
    
    <published>2010-07-24T07:05:04Z</published>
    <updated>2010-07-24T07:05:04Z</updated>
    <content type="html">

&lt;div class=WordSection1&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;HUBBLE
SPACE TELESCOPE - Continuing to Collect World Class Science &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;DAILY
REPORT #5144 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;PERIOD
COVERED: 5am July 22 - 5am July 23, 2010 (DOY 203/09:00z-204/09:00z) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;FLIGHT
OPERATIONS SUMMARY: &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Significant
Spacecraft Anomalies: (The following are preliminary reports&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;of
potential non-nominal performance that will be investigated.) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;HSTARS:
(None) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COMPLETED
OPS REQUEST: (None) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COMPLETED
OPS NOTES: (None) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;SCHEDULED&amp;#160;&amp;#160; SUCCESSFUL&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;FGS
GSAcq&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;6&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
6&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;FGS
REAcq&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;9&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
9&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;OBAD with
Maneuver&amp;#160;&amp;#160;&amp;#160;&amp;#160;
6&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
6&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;SIGNIFICANT
EVENTS: (None) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;OBSERVATIONS
SCHEDULED: &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COS/NUV
11894 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;NUV Detector
Dark Monitor &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;The purpose
of this proposal is to measure the NUV detector dark rate by&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;taking long
science exposures with no light on the detector. The&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;detector
dark rate and spatial distribution of counts will be compared&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;to
pre-launch and SMOV data in order to verify the nominal operation of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the
detector. Variations of count rate as a function of orbital position&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;will be
analyzed to find dependence of dark rate on proximity to the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;SAA. Dependence
of dark rate as function of time will also be tracked. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COS/NUV/FUV
11728 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;The Impact
of Starbursts on the Gaseous Halos of Galaxies &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Perhaps the
most important (yet uncertain) aspects of galaxy evolution&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;are the
processes by which galaxies accrete gas and by which the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;resulting
star formation and black hole growth affects this accreting&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;gas. It is
believed that both the form of the accretion and the nature&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;of the
feedback change as a function of the galaxy mass. At low mass the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;gas comes
in cold and the feedback is provided by massive stars. At high&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;mass, the
gas comes in hot, and the feedback is from an AGN. The&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;changeover
occurs near the mass where the galaxy population transitions&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;from
star-forming galaxies to red and dead ones. The population of red&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;and dead
galaxies is building with cosmic time, and it is believed that&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;feedback
plays an important role in this process: shutting down star&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;formation
by heating and/or expelling the reservoir of cold halo gas. To&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;investigate
these ideas, we propose to use COS far-UV spectra of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;background
QSOs to measure the properties of the halo gas in a sample of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;galaxies
near the transition mass that have undergone starbursts within&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the past
100 Myr to 1 Gyr. The galactic wind associated with the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;starburst
is predicted to have affected the properties of the gaseous&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;halo. To
test this, we will compare the properties of the halos of the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;post-starburst
galaxies to those of a control sample of galaxies matched&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;in mass and
QSO impact parameter. Do the halos of the post-starburst&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;galaxies
show a higher incidence rate of Ly-Alpha and metal&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;absorption-lines?
Are the kinematics of the halo gas more disturbed in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the
post-starbursts? Has the wind affected the ionization state and/or&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the metallicity
of the halo? These data will provide fresh new insights&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;into the
role of feedback from massive stars on the evolution of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;galaxies,
and may also offer clues about the properties of the QSO metal&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;absorption-line
systems at high-redshift . &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;STIS/CC
11845 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;CCD Dark
Monitor Part 2 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Monitor the
darks for the STIS CCD. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;STIS/CC
11847 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;CCD Bias
Monitor-Part 2 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Monitor the
bias in the 1x1, 1x2, 2x1, and 2x2 bin settings at gain=1,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;and 1x1 at
gain = 4, to build up high-S/N superbiases and track the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;evolution
of hot columns. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;STIS/MA1/MA2
11857 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;STIS Cycle
17 MAMA Dark Monitor &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;This
proposal monitors the behavior of the dark current in each of the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;MAMA
detectors. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;The basic
monitor takes two 1380s ACCUM darks each week with each&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;detector. However,
starting Oct 5, pairs are only included for weeks&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;that the
LRP has external MAMA observations planned. The weekly pairs of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;exposures
for each detector are linked so that they are taken at&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;opposite
ends of the same SAA free interval. This pairing of exposures&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;will make
it easier to separate long and short term temporal variability&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;from
temperature dependent changes. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;For both
detectors, additional blocks of exposures are taken once every&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;six months.
These are groups of five 1314s FUV-MAMA Time-Tag darks or&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;five 3x315s
NUV ACCUM darks distributed over a single SAA-free interval.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;This will
give more information on the brightness of the FUV MAMA dark&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;current as
a function of the amount of time that the HV has been on, and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;for the NUV
MAMA will give a better measure of the short term&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;temperature
dependence. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/ACS/UVIS
11613 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;GHOSTS:
Stellar Outskirts of Massive Spiral Galaxies &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;We propose
to continue our highly successful GHOSTS HST survey of the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;resolved
stellar populations of nearby, massive disk galaxies using&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;SNAPs.
These observations provide star counts and color-magnitude&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;diagrams
2-3 magnitudes below the tip of the Red Giant Branch of the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;outer disk
and halo of each galaxy. We will measure the metallicity&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;distribution
functions and stellar density profiles from star counts&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;down to
very low average surface brightnesses, equivalent to ~32 V-mag&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;per square
arcsec. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;This
proposal will substantially improve our unique sampling of galaxy&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;outskirts. Our
targets cover a range in galaxy mass, luminosity,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;inclination,
and morphology. As a function of these galaxy properties,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;this survey
provides: - the most extensive, systematic measurement of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;radial
light profiles and axial ratios of the diffuse stellar halos and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;outer disks
of spiral galaxies; - a comprehensive analysis of halo&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;metallicity
distributions as function of galaxy type and position within&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the galaxy;
- an unprecedented study of the stellar metallicity and age&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;distribution
in the outer disk regions where the disk truncations occur;&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;- the first
comparative study of globular clusters and their field&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;stellar
populations. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;We will use
these fossil records of the galaxy assembly process to test&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;halo
formation models within the hierarchical galaxy formation scheme. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/IR
11696 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Infrared
Survey of Star Formation Across Cosmic Time &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;We propose
to use the unique power of WFC3 slitless spectroscopy to&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;measure the
evolution of cosmic star formation from the end of the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;reionization
epoch at z&amp;#62;6 to the close of the galaxy- building era at&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;z~0.3.Pure
parallel observations with the grisms have proven to be&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;efficient
for identifying line emission from galaxies across a broad&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;range of
redshifts. The G102 grism on WFC3 was designed to extend this&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;capability
to search for Ly-alpha emission from the first galaxies.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Using up to
250 orbits of pure parallel WFC3 spectroscopy, we will&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;observe
about 40 deep (4-5 orbit) fields with the combination of G102&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;and G141,
and about 20 shallow (2-3 orbit) fields with G141 alone. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Our primary
science goals at the highest redshifts are: (1) Detect Lya&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;in ~100
galaxies with z&amp;#62;5.6 and measure the evolution of the Lya&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;luminosity
function, independent of of cosmic variance; 2) Determine the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;connection between
emission line selected and continuum-break selected&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;galaxies at
these high redshifts, and 3) Search for the proposed&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;signature
of neutral hydrogen absorption at re-ionization. At&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;intermediate
redshifts we will (4) Detect more than 1000 galaxies in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Halpha at
0.5&amp;#60;z&amp;#60;1.8 to measure the evolution of the extinction-corrected&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;star
formation density across the peak epoch of star formation. This is&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;over an
order-of-magnitude improvement in the current statistics, from&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the NICMOS
Parallel grism survey. (5) Trace ``cosmic downsizing&amp;#34; from&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;0.5&amp;#60;z&amp;#60;2.2;
and (6) Estimate the evolution in reddening and metallicty in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;star-
forming galaxies and measure the evolution of the Seyfert&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;population.
For hundreds of spectra we will be able to measure one or&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;even two
line pair ratios -- in particular, the Balmer decrement and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;/
are sensitive to gas reddening and metallicity. As a bonus,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the G102
grism offers the possibility of detecting Lya emission at&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;z=7-8.8. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;To identify
single-line Lya emitters, we will exploit the wide&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;0.8--1.9um
wavelength coverage of the combined G102+G141 spectra. All&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt; and
 interlopers detected in G102 will be reliably separated&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;from true
LAEs by the detection of at least one strong line in the G141&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;spectrum,
without the need for any ancillary data. We waive all&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;proprietary
rights to our data and will make high-level data products&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;available
through the ST/ECF. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/IR
11915 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;IR Internal
Flat Fields &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;This
program is the same as 11433 (SMOV) and depends on the completion&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;of the IR initial
alignment (Program 11425). This version contains three&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;instances
of 37 internal orbits: to be scheduled early, middle, and near&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the end of
Cycle 17, in order to use the entire 110-orbit allocation. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;In this
test, we will study the stability and structure of the IR&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;channel
flat field images through all filter elements in the WFC3-IR&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;channel.
Flats will be monitored, i.e. to capture any temporal trends in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the flat
fields and delta flats produced. High signal observations will&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;provide a
map of the pixel-to-pixel flat field structure, as well as&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;identify
the positions of any dust particles. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/IR/S/C
11929 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;IR Dark
Current Monitor &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Analyses of
ground test data showed that dark current signals are more&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;reliably
removed from science data using darks taken with the same&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;exposure
sequences as the science data, than with a single dark current&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;image
scaled by desired exposure time. Therefore, dark current images&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;must be
collected using all sample sequences that will be used in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;science
observations. These observations will be used to monitor changes&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;in the dark
current of the WFC3-IR channel on a day-to-day basis, and to&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;build
calibration dark current ramps for each of the sample sequences to&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;be used by
Gos in Cycle 17. For each sample sequence/array size&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;combination,
a median ramp will be created and delivered to the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;calibration
database system (CDBS). &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UV/ACS/WFC/IR
12058 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;A
Panchromatic Hubble Andromeda Treasury - I &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;We propose
to image the north east quadrant of M31 to deep limits in the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;UV, optical,
and near-IR. HST imaging should resolve the galaxy into&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;more than
100 million stars, all with common distances and foreground&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;extinctions.
UV through NIR stellar photometry (F275W, F336W with&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UVIS,
F475W and F814W with ACS/WFC, and F110W and F160W with&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/NIR)
will provide effective temperatures for a wide range of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;spectral
types, while simultaneously mapping M31's extinction. Our&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;central
science drivers are to: understand high-mass variations in the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;stellar IMF
as a function of SFR intensity and metallicity; capture the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;spatially-resolved
star formation history of M31; study a vast sample of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;stellar
clusters with a range of ages and metallicities. These are&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;central to
understanding stellar evolution and clustered star formation;&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;constraining
ISM energetics; and understanding the counterparts and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;environments
of transient objects (novae, SNe, variable stars, x-ray&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;sources,
etc.). As its legacy, this survey adds M31 to the Milky Way and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Magellanic
Clouds as a fundamental calibrator of stellar evolution and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;star-formation
processes for understanding the stellar populations of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;distant
galaxies. Effective exposure times are 977s in F275W, 1368s in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;F336W,
4040s in F475W, 4042s in F814W, 699s in F110W, and 1796s in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;F160W,
including short exposures to avoid saturation of bright sources.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;These
depths will produce photon-limited images in the UV. Images will&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;be
crowding-limited in the optical and NIR, but will reach below the red&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;clump at
all radii. The images will reach the Nyquist sampling limit in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;F160W,
F475W, and F814W. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UVIS
11643 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;A Timeline
for Early-Type Galaxy Formation: Mapping the Evolution of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Star
Formation, Globular Clusters, Dust, and Black Holes &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;While
considerable effort has been devoted to statistical studies of the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;origin of the
red sequence of galaxies, there has been relatively little&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;direct
exploration of galaxies transforming from late to early types.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Such
galaxies are identified by their post-starburst spectra, bulge-&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;dominated,
tidally-disturbed morphologies, and current lack of gas. We&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;are
constructing the first detailed timeline of their evolution onto the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;red
sequence, pinpointing when star formation ends, nuclear activity&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;ceases,
globular clusters form, and the bulk of the merging progenitors'&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;dust
disappears. Here we propose to obtain HST and Chandra imaging of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;nine
galaxies, whose wide range of post-starburst ages we have precisely&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;dated with
a new UV-optical technique and for which we were awarded&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Spitzer
time. We will address 1) whether the black hole-bulge mass&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;relation
arises from nuclear feedback, 2) whether the bimodality of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;globular
cluster colors is due to young clusters produced in galaxy&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;mergers,
and 3) what happens to the dust when late types merge to form&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;an early
type. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UVIS
11905 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3 UVIS
CCD Daily Monitor &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;The
behavior of the WFC3 UVIS CCD will be monitored daily with a set of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;full-frame,
four-amp bias and dark frames. A smaller set of 2Kx4K&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;subarray
biases are acquired at less frequent intervals throughout the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;cycle to support
subarray science observations. The internals from this&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;proposal,
along with those from the anneal procedure (Proposal 11909),&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;will be
used to generate the necessary superbias and superdark reference&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;files for
the calibration pipeline (CDBS). &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UVIS
11907 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;UVIS Cycle
17 Contamination Monitor &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;The UV
throughput of WFC3 during Cycle 17 is monitored via weekly&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;standard
star observations in a subset of key filters covering 200-600nm&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;and F606W,
F814W as controls on the red end. The data will provide a&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;measure of
throughput levels as a function of time and wavelength,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;allowing
for detection of the presence of possible contaminants. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UVIS
11908 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Cycle 17:
UVIS Bowtie Monitor &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Ground
testing revealed an intermittent hysteresis type effect in the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;UVIS
detector (both CCDs) at the level of ~1%, lasting hours to days.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Initially
found via an unexpected bowtie-shaped feature in flatfield&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;ratios,
subsequent lab tests on similar e2v devices have since shown&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;that it is
also present as simply an overall offset across the entire&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;CCD, i.e.,
a QE offset without any discernable pattern. These lab tests&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;have
further revealed that overexposing the detector to count levels&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;several
times full well fills the traps and effectively neutralizes the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;bowtie.
Each visit in this proposal acquires a set of three 3x3 binned&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;internal
flatfields: the first unsaturated image will be used to detect&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;any bowtie,
the second, highly exposed image will neutralize the bowtie&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;if it is present,
and the final image will allow for verification that&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the bowtie
is gone.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/p&gt;

&lt;p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto'&gt;&lt;span
style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;color:black'&gt;-&lt;/span&gt;&lt;span
style='font-size:10.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;color:black'&gt;Lynn&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&lt;/span&gt;&lt;b&gt;&lt;span style='font-family:&quot;Arial&quot;,&quot;sans-serif&quot;'&gt;&amp;#160;&amp;#160;&amp;#160;&lt;/span&gt;&lt;/b&gt;&lt;span
style='color:#1F497D'&gt;&lt;img width=123 height=99 id=&quot;Picture_x0020_1&quot;
src=&quot;cid:&amp;#105;&amp;#109;&amp;#x61;&amp;#103;&amp;#x65;&amp;#48;&amp;#48;&amp;#49;&amp;#x2E;&amp;#x6A;&amp;#x70;&amp;#x67;&amp;#64;&amp;#x30;&amp;#x31;&amp;#x43;&amp;#x42;&amp;#x32;&amp;#65;&amp;#56;&amp;#51;&amp;#46;&amp;#x41;&amp;#51;&amp;#x41;&amp;#x32;&amp;#53;&amp;#66;&amp;#x43;&amp;#x30;&quot;
alt=&quot;cid:&amp;#x69;&amp;#109;&amp;#x61;&amp;#103;&amp;#101;&amp;#x30;&amp;#x30;&amp;#49;&amp;#x2E;&amp;#x6A;&amp;#112;&amp;#x67;&amp;#x40;&amp;#x30;&amp;#49;&amp;#x43;&amp;#x41;&amp;#52;&amp;#55;&amp;#x32;&amp;#x44;&amp;#x2E;&amp;#x43;&amp;#67;&amp;#x41;&amp;#x36;&amp;#57;&amp;#x34;&amp;#x44;&amp;#48;&quot;&gt;&lt;/span&gt;&lt;span style='color:black'&gt;&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto'&gt;&lt;span
style='font-size:10.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;color:black'&gt;NASA
office: 301-286-2876&lt;/span&gt;&lt;span style='color:black'&gt; &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto'&gt;&lt;span
style='font-size:10.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;color:black'&gt;__________________________________________________________&lt;br&gt;
Lynn F. Bassford&lt;br&gt;
&lt;/span&gt;&lt;span style='font-size:10.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;
color:blue'&gt;Hubble &lt;/span&gt;&lt;span style='font-size:10.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;
color:red'&gt;Space &lt;/span&gt;&lt;span style='font-size:10.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;
color:purple'&gt;Telescope&lt;br&gt;
&lt;/span&gt;&lt;span style='font-size:10.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;
color:black'&gt;CHAMP Mission Operations Manager&lt;/span&gt;&lt;span style='font-size:
10.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;color:purple'&gt;&lt;br&gt;
&lt;/span&gt;&lt;span style='font-size:10.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;
color:black'&gt;CHAMP Flight Operations Team Manager&lt;br&gt;
Lockheed Martin Mission Services (LMMS) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='color:black'&gt;&amp;#34;...Hubble is the most
significant science instrument of all time in terms of its
productivity...&amp;#34; &amp;#160;&amp;#160;&amp;#160;&amp;#160;Scott Altman @12:45pm 5/21/9
STS-125 Senate Subcommittee Hearing&lt;/span&gt;&lt;o:p&gt;&lt;/o:p&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/p&gt;

&lt;/div&gt;








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  <entry>
    <title>sci.astro.hubble - 2 new messages in 2 topics - digest</title>
    <link rel="alternate" href="http://www.aus-city.com/cgi-bin/dada/mail.cgi/archive/HST_REPORTS/20100723180502/"/>
    <id>tag:www.aus-city.com,2010-07-23:%2Fcgi-bin%2Fdada%2Fmail.cgi%2Farchive%2FHST_REPORTS%2F20100723180502%2F</id>
    
    <published>2010-07-23T18:05:02Z</published>
    <updated>2010-07-23T18:05:02Z</updated>
    <content type="html">
 
&lt;p&gt;sci.astro.hubble&lt;br/&gt;
&lt;a href=&quot;http://groups.google.com/group/sci.astro.hubble?hl=en&quot;&gt;http://groups.google.com/group/sci.astro.hubble?hl=en&lt;/a&gt;
&lt;/p&gt;&lt;p&gt;&lt;a href=&quot;mailto:&amp;#115;&amp;#x63;&amp;#x69;&amp;#x2E;&amp;#x61;&amp;#x73;&amp;#116;&amp;#114;&amp;#111;&amp;#46;&amp;#x68;&amp;#x75;&amp;#98;&amp;#98;&amp;#108;&amp;#x65;&amp;#x40;&amp;#103;&amp;#x6F;&amp;#x6F;&amp;#103;&amp;#108;&amp;#x65;&amp;#103;&amp;#x72;&amp;#111;&amp;#117;&amp;#x70;&amp;#115;&amp;#x2E;&amp;#x63;&amp;#111;&amp;#x6D;&quot;&gt;&amp;#115;&amp;#x63;&amp;#x69;&amp;#x2E;&amp;#x61;&amp;#x73;&amp;#116;&amp;#114;&amp;#111;&amp;#46;&amp;#x68;&amp;#x75;&amp;#98;&amp;#98;&amp;#108;&amp;#x65;&amp;#x40;&amp;#103;&amp;#x6F;&amp;#x6F;&amp;#103;&amp;#108;&amp;#x65;&amp;#103;&amp;#x72;&amp;#111;&amp;#117;&amp;#x70;&amp;#115;&amp;#x2E;&amp;#x63;&amp;#111;&amp;#x6D;&lt;/a&gt;
&lt;/p&gt;&lt;p&gt;Today's topics:
&lt;/p&gt;&lt;ul&gt;
  &lt;li&gt;Daily Report #5142 - 1 messages, 1 author
 &lt;a href=&quot;http://groups.google.com/group/sci.astro.hubble/t/5d7f4a3cadc34dd3?hl=en&quot;&gt;http://groups.google.com/group/sci.astro.hubble/t/5d7f4a3cadc34dd3?hl=en&lt;/a&gt;
  &lt;/li&gt;&lt;li&gt;Daily Report #5143 - 1 messages, 1 author
 &lt;a href=&quot;http://groups.google.com/group/sci.astro.hubble/t/1e70a960d2b675f4?hl=en&quot;&gt;http://groups.google.com/group/sci.astro.hubble/t/1e70a960d2b675f4?hl=en&lt;/a&gt;&lt;/li&gt;&lt;/ul&gt;
&lt;hr/&gt;
TOPIC: Daily Report #5142&lt;br/&gt;
&lt;a href=&quot;http://groups.google.com/group/sci.astro.hubble/t/5d7f4a3cadc34dd3?hl=en&quot;&gt;http://groups.google.com/group/sci.astro.hubble/t/5d7f4a3cadc34dd3?hl=en&lt;/a&gt;
&lt;hr/&gt;
&lt;p&gt;== 1 of 1 ==&lt;br/&gt;
Date: Wed, Jul 21 2010 8:14&amp;#194;&amp;#160;am 
From: &amp;#34;Bassford, Lynn&amp;#34;  
&lt;/p&gt;
&lt;p&gt;HUBBLE SPACE TELESCOPE - Continuing to Collect World Class Science
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;DAILY REPORT #5142&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;PERIOD COVERED: 5am July 20 - 5am July 21, 2010 (DOY 201/09:00z-202/09:00z)
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;FLIGHT OPERATIONS SUMMARY:&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Significant Spacecraft Anomalies: (The following are preliminary
reports of potential non-nominal performance that will be
investigated.)
&lt;/p&gt;&lt;dl&gt;
  &lt;dt&gt;HSTARS&lt;/dt&gt;
&lt;dd&gt;&lt;/dd&gt;&lt;/dl&gt;
&lt;p&gt;From DOY 188:
&lt;/p&gt;&lt;p&gt;#12336 GSAcq(2,1,1) @188/14:11:27z required two attempts to achieve
CT-DV on FGS2. The acquisition was successful.
&lt;/p&gt;&lt;p&gt;COMPLETED OPS REQUEST: (None)
&lt;/p&gt;&lt;p&gt;COMPLETED OPS NOTES: (None)
&lt;/p&gt;&lt;pre&gt;
                             SCHEDULED      SUCCESSFUL
FGS GSAcq                     5                5
FGS REAcq                    11               11
OBAD with Maneuver            6                6&lt;/pre&gt;
&lt;p&gt;SIGNIFICANT EVENTS: (None)
&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;OBSERVATIONS SCHEDULED:&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;ACS/WFC3 11833&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Monitoring M31 for BHXNe
&lt;/p&gt;&lt;p&gt;During A01-8 we found ~20 Black Hole X-ray Novae (BHXNe) in M31 using
Chandra, and with HST follow-up have estimated orbital periods for 8
of these. Observations are underway with HST to attempt to estimate
additional periods. We propose to continue this program concentrating
our scarce HST resources on a single transient which exceeds 1e38
erg/s. Only uninterrupted monitoring can yield the duty cycles and
long-term light curves of BHXNe (and other variables) in M31. Our
GO+GTO programs will have accumulated 790ks (ACIS+HRC) near the M31
bulge by the end of AO9, and total Chandra exposure on M31 is now
940ks. By continuing our monitoring program through AO12 we will reach
~950ks on the bulge and &amp;#62;1Msec total Chandra M31 exposure.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;COS/FUV 11527&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;COS-GTO: An Absorption Study of Galactic Intermediate Velocity Clouds
Using Hot Stars in Globular Clusters
&lt;/p&gt;&lt;p&gt;We shall use UV bright hot post-AGB stars located within the globular
clusters of NGC 5139, NGC 6752, NGC 7078, NGC 6205, NGC 5272 and NGC
1904 to sample the UV absorption properties of the intervening
line-of-sight interstellar gas. Such sight-lines pass through several
intermediate velocity clouds (IVC?s) thought to be located within 5
kpc of our Galaxy, thus allowing the physical and chemical state of
this gas to be probed and compared with the properties of interstellar
gas located in the galactic disk. Elemental abundances of the IVC gas
shall be derived in order to determine a possible origin for these
in-falling galactic satellite cloud structures.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;COS/FUV 11686&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;The Cosmological Impact of AGN Outflows: Measuring Absolute Abundances
and Kinetic Luminosities
&lt;/p&gt;&lt;p&gt;AGN outflows are increasingly invoked as a major contributor to the
formation and evolution of supermassive black holes, their host
galaxies, the surrounding IGM, and cluster cooling flows. Our HST/COS
proposal will determine reliable absolute chemical abundances in six
AGN outflows, which influences several of the processes mentioned
above. To date there is only one such determination, done by our team
on Mrk 279 using 16 HST/STIS orbits and 100 ksec of FUSE time. The
advent of COS and its high sensitivity allows us to choose among
fainter objects at redshifts high enough to preclude the need for
FUSE. This will allow us to determine the absolute abundances for six
AGN (all fainter than Mrk 279) using only 40 HST COS orbits. This will
put abundances studies in AGN on a firm footing, an elusive goal for
the past four decades. In addition, prior FUSE observations of four of
these targets indicate that it is probable that the COS observations
will detect troughs from excited levels of C III. These will allow us
to measure the distances of the outflows and thereby determine their
kinetic luminosity, a major goal in AGN feedback research.
&lt;/p&gt;&lt;p&gt;We will use our state of the art column density extraction methods and
velocity-dependent photoionization models to determine the abundances
and kinetic luminosity. Previous AGN outflow projects suffered from
the constraints of deciding what science we could do using ONE of the
handful of bright targets that were observable. With COS we can choose
the best sample for our experiment. As an added bonus, most of the
spectral range of our targets has not been observed previously,
greatly increasing the discovery phase space.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/CC 11845&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;CCD Dark Monitor Part 2
&lt;/p&gt;&lt;p&gt;Monitor the darks for the STIS CCD.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/CC 11847&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;CCD Bias Monitor-Part 2
&lt;/p&gt;&lt;p&gt;Monitor the bias in the 1x1, 1x2, 2x1, and 2x2 bin settings at gain=1,
and 1x1 at gain = 4, to build up high-S/N superbiases and track the
evolution of hot columns.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/CCD 11721&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Verifying the Utility of Type Ia Supernovae as Cosmological Probes:
Evolution and Dispersion in the Ultraviolet Spectra
&lt;/p&gt;&lt;p&gt;The study of distant type Ia supernova (SNe Ia) offers the most
practical and immediate discriminator between popular models of dark
energy. Yet fundamental questions remain over possible
redshift-dependent trends in their observed and intrinsic properties.
High-quality Keck spectroscopy of a representative sample of 36
intermediate redshift SNe Ia has revealed a surprising, and
unexplained, diversity in their rest-frame UV fluxes. One possible
explanation is hitherto undiscovered variations in the progenitor
metallicity. Unfortunately, this result cannot be compared to local UV
data as only two representative SNe Ia have been studied near maximum
light. Taking advantage of two new `rolling searches' and the
restoration of STIS, we propose a non-disruptive TOO campaign to
create an equivalent comparison local sample. This will allow us to
address possible evolution in the mean UV spectrum and its diversity,
an essential precursor to the study of SNe beyond z~1.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/IR 11712&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Calibration of Surface Brightness Fluctuations for WFC3/IR
&lt;/p&gt;&lt;p&gt;We aim to characterize galaxy surface brightness fluctuations (SBF),
and calibrate the SBF distance method, in the F110W and F160W filters
of the Wide Field Camera 3 IR channel. Because of the very high
throughput of F110W and the good match of F160W to the standard H
band, we anticipate that both of these filters will be popular choices
for galaxy observations with WFC3/IR. The SBF signal is typically an
order of magnitude brighter in the near-IR than in the optical, and
the characteristics (sensitivity, FOV, cosmetics) of the WFC3/IR
channel will be enormously more efficient for SBF measurements than
previously available near-IR cameras. As a result, our proposed SBF
calibration will allow accurate distance derivation whenever an
early-type or bulge-dominated galaxy is observed out to a distance of
150 Mpc or more (i.e., out to the Hubble flow) in the calibrated
passbands. For individual galaxy observations, an accurate distance is
useful for establishing absolute luminosities, black hole masses,
linear sizes, etc. Eventually, once a large number of galaxies have
been observed across the sky with WFC3/IR, this SBF calibration will
enable accurate mapping of the total mass density distribution in the
local universe using the data available in the HST archive. The
proposed observations will have additional important scientific value;
in particular, we highlight their usefulness for understanding the
nature of multimodal globular cluster color distributions in giant
elliptical galaxies.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/IR/S/C 11929&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;IR Dark Current Monitor
&lt;/p&gt;&lt;p&gt;Analyses of ground test data showed that dark current signals are more
reliably removed from science data using darks taken with the same
exposure sequences as the science data, than with a single dark
current image scaled by desired exposure time. Therefore, dark current
images must be collected using all sample sequences that will be used
in science observations. These observations will be used to monitor
changes in the dark current of the WFC3-IR channel on a day-to-day
basis, and to build calibration dark current ramps for each of the
sample sequences to be used by Gos in Cycle 17. For each sample
sequence/array size combination, a median ramp will be created and
delivered to the calibration database system (CDBS).
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UVIS 11697&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Proper Motion Survey of Classical and SDSS Local Group Dwarf Galaxies
&lt;/p&gt;&lt;p&gt;Using the superior resolution of HST, we propose to continue our
proper motion survey of Galactic dwarf galaxies. The target galaxies
include one classical dwarf, Leo II, and six that were recently
identified in the Sloan Digital Sky Survey data: Bootes I, Canes
Venatici I, Canes Venatici II, Coma Berenices, Leo IV, and Ursa Major
II. We will observe a total of 16 fields, each centered on a
spectroscopically-confirmed QSO. Using QSOs as standards of rest in
measuring absolute proper motions has proven to be the most accurate
and most efficient method. HST is our only option to quickly determine
the space motions of the SDSS dwarfs because suitable ground-based
imaging is only a few years old and such data need several decades to
produce a proper motion. The two most distant galaxies in our sample
will require time baselines of four years to achieve our goal of a
30-50 km/s uncertainty in the tangential velocity; given this and the
finite lifetime of HST, it is imperative that first-epoch observations
be taken in this cycle. The SDSS dwarfs have dramatically lower
surface brightnesses and luminosities than the classical dwarfs.
Proper motions are crucial for determining orbits of the galaxies and
knowing the orbits will allow us to test theories for the formation
and evolution of these galaxies and, more generally, for the formation
of the Local Group.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UVIS 11905&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;WFC3 UVIS CCD Daily Monitor
&lt;/p&gt;&lt;p&gt;The behavior of the WFC3 UVIS CCD will be monitored daily with a set
of full-frame, four-amp bias and dark frames. A smaller set of 2Kx4K
subarray biases are acquired at less frequent intervals throughout the
cycle to support subarray science observations. The internals from
this proposal, along with those from the anneal procedure (Proposal
11909), will be used to generate the necessary superbias and superdark
reference files for the calibration pipeline (CDBS).
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UVIS/IR 11644&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;A Dynamical-Compositional Survey of the Kuiper Belt: A New Window Into
the Formation of the Outer Solar System
&lt;/p&gt;&lt;p&gt;The eight planets overwhelmingly dominate the solar system by mass,
but their small numbers, coupled with their stochastic pasts, make it
impossible to construct a unique formation history from the dynamical
or compositional characteristics of them alone. In contrast, the huge
numbers of small bodies scattered throughout and even beyond the
planets, while insignificant by mass, provide an almost unlimited
number of probes of the statistical conditions, history, and
interactions in the solar system. To date, attempts to understand the
formation and evolution of the Kuiper Belt have largely been dynamical
simulations where a hypothesized starting condition is evolved under
the gravitational influence of the early giant planets and an attempt
is made to reproduce the current observed populations. With little
compositional information known for the real Kuiper Belt, the test
particles in the simulation are free to have any formation location
and history as long as they end at the correct point. Allowing
compositional information to guide and constrain the formation,
thermal, and collisional histories of these objects would add an
entire new dimension to our understanding of the evolution of the
outer solar system. While ground based compositional studies have hit
their flux limits already with only a few objects sampled, we propose
to exploit the new capabilities of WFC3 to perform the first ever
large-scale dynamical-compositional study of Kuiper Belt Objects
(KBOs) and their progeny to study the chemical, dynamical, and
collisional history of the region of the giant planets. The
sensitivity of the WFC3 observations will allow us to go up to two
magnitudes deeper than our ground based studies, allowing us the
capability of optimally selecting a target list for a large survey
rather than simply taking the few objects that can be measured, as we
have had to do to date. We have carefully constructed a sample of 120
objects which provides both overall breadth, for a general
understanding of these objects, plus a large enough number of objects
in the individual dynamical subclass to allow detailed comparison
between and within these groups. These objects will likely define the
core Kuiper Belt compositional sample for years to come. While we have
many specific results anticipated to come from this survey, as with
any project where the field is rich, our current knowledge level is
low, and a new instrument suddenly appears which can exploit vastly
larger segments of the population, the potential for discovery -- both
anticipated and not -- is extraordinary.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UVIS/IR 11909&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;UVIS Hot Pixel Anneal
&lt;/p&gt;&lt;p&gt;The on-orbit radiation environment of WFC3 will continually generate
new hot pixels. This proposal performs the procedure required for
repairing those hot pixels in the UVIS CCDs. During an anneal, the
two-stage thermo-electric cooler (TEC) is turned off and the
four-stage TEC is used as a heater to bring the UVIS CCDs up to ~20
deg. C. As a result of the CCD warmup, a majority of the hot pixels
will be fixed; previous instruments such as WFPC2 and ACS have seen
repair rates of about 80%. Internal UVIS exposures are taken before
and after each anneal, to allow an assessment of the procedure's
effectiveness in WFC3, provide a check of bias, global dark current,
and hot pixel levels, as well as support hysteresis (bowtie)
monitoring and CDBS reference file generation. One IR dark is taken
after each anneal, to provide a check of the IR detector.
&lt;/p&gt;


&lt;hr/&gt;
TOPIC: Daily Report #5143&lt;br/&gt;
&lt;a href=&quot;http://groups.google.com/group/sci.astro.hubble/t/1e70a960d2b675f4?hl=en&quot;&gt;http://groups.google.com/group/sci.astro.hubble/t/1e70a960d2b675f4?hl=en&lt;/a&gt;
&lt;hr/&gt;
&lt;p&gt;== 1 of 1 ==&lt;br/&gt;
Date: Thurs, Jul 22 2010 6:38&amp;#194;&amp;#160;am 
From: &amp;#34;Bassford, Lynn&amp;#34;  
&lt;/p&gt;
&lt;p&gt;HUBBLE SPACE TELESCOPE - Continuing to Collect World Class Science
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;DAILY REPORT #5143&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;PERIOD COVERED: 5am July 21 - 5am July 22, 2010 (DOY 202/09:00z-203/09:00z)
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;FLIGHT OPERATIONS SUMMARY:&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Significant Spacecraft Anomalies: (The following are preliminary 
reports of potential non-nominal performance that will be 
investigated.)
&lt;/p&gt;&lt;p&gt;HSTARS: (None)
&lt;/p&gt;&lt;p&gt;COMPLETED OPS REQUEST: (None)
&lt;/p&gt;&lt;p&gt;COMPLETED OPS NOTES: (None)
&lt;/p&gt;&lt;pre&gt;
                       SCHEDULED      SUCCESSFUL
FGS GSAcq                 7                7
FGS REAcq                 9                9
OBAD with Maneuver        3                3&lt;/pre&gt;
&lt;p&gt;SIGNIFICANT EVENTS: (None)
&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;OBSERVATIONS SCHEDULED:&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;ACS/WFC 11996&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;CCD Daily Monitor (Part 3)
&lt;/p&gt;&lt;p&gt;This program comprises basic tests for measuring the read noise and 
dark current of the ACS WFC and for tracking the growth of hot pixels. 
The recorded frames are used to create bias and dark reference images 
for science data reduction and calibration. This program will be 
executed four days per week (Mon, Wed, Fri, Sun) for the duration of 
Cycle 17. To facilitate scheduling, this program is split into three 
proposals. This proposal covers 308 orbits (19.25 weeks) from 21 June 
2010 to 1 November 2010.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/CC 11845&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;CCD Dark Monitor Part 2
&lt;/p&gt;&lt;p&gt;Monitor the darks for the STIS CCD.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/CC 11847&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;CCD Bias Monitor-Part 2
&lt;/p&gt;&lt;p&gt;Monitor the bias in the 1x1, 1x2, 2x1, and 2x2 bin settings at gain=1, 
and 1x1 at gain = 4, to build up high-S/N superbiases and track the 
evolution of hot columns.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/CC/MA 11668&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Cosmo-chronometry and Elemental Abundance Distribution of the Ancient
Star HE1523-0901
&lt;/p&gt;&lt;p&gt;We propose to obtain near-UV HST/STIS spectroscopy of the extremely 
metal-poor, highly r-process-enhanced halo star HE 1523-0901, in order 
to produce the most complete abundance distribution of the heaviest 
stable elements, including platinum, osmium, and lead. These HST 
abundance data will then be used to estimate the initial abundances of 
the long-lived radioactive elements thorium and uranium, and by 
comparison with their observed abundances, enable an accurate age 
determination of this ancient star. The use of radioactive 
chronometers in stars provides an independent lower limit on the age 
of the Galaxy, which can be compared with alternative limits set by 
globular clusters and by analysis from WMAP. Our proposed observations 
of HE1523-0901 will also provide significant new information about the 
early chemical history of the Galaxy, specifically, the nature of the 
first generations of stars and the types of nucleosynthetic processes 
that occurred at the onset of Galactic chemical evolution.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/MA1/MA2 11857&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;STIS Cycle 17 MAMA Dark Monitor
&lt;/p&gt;&lt;p&gt;This proposal monitors the behavior of the dark current in each of the 
MAMA detectors.
&lt;/p&gt;&lt;p&gt;The basic monitor takes two 1380s ACCUM darks each week with each 
detector. However, starting Oct 5, pairs are only included for weeks 
that the LRP has external MAMA observations planned. The weekly pairs 
of exposures for each detector are linked so that they are taken at 
opposite ends of the same SAA free interval. This pairing of exposures 
will make it easier to separate long and short term temporal 
variability from temperature dependent changes.
&lt;/p&gt;&lt;p&gt;For both detectors, additional blocks of exposures are taken once 
every six months. These are groups of five 1314s FUV-MAMA Time-Tag 
darks or five 3x315s NUV ACCUM darks distributed over a single 
SAA-free interval. This will give more information on the brightness 
of the FUV MAMA dark current as a function of the amount of time that 
the HV has been on, and for the NUV MAMA will give a better measure of 
the short term temperature dependence.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UV/ACS/WFC/IR 12058&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;A Panchromatic Hubble Andromeda Treasury - I
&lt;/p&gt;&lt;p&gt;We propose to image the north east quadrant of M31 to deep limits in 
the UV, optical, and near-IR. HST imaging should resolve the galaxy 
into more than 100 million stars, all with common distances and 
foreground extinctions. UV through NIR stellar photometry (F275W, 
F336W with WFC3/UVIS, F475W and F814W with ACS/WFC, and F110W and 
F160W with WFC3/NIR) will provide effective temperatures for a wide 
range of spectral types, while simultaneously mapping M31's 
extinction. Our central science drivers are to: understand high-mass 
variations in the stellar IMF as a function of SFR intensity and 
metallicity; capture the spatially-resolved star formation history of 
M31; study a vast sample of stellar clusters with a range of ages and 
metallicities. These are central to understanding stellar evolution 
and clustered star formation; constraining ISM energetics; and 
understanding the counterparts and environments of transient objects 
(novae, SNe, variable stars, x-ray sources, etc.). As its legacy, this 
survey adds M31 to the Milky Way and Magellanic Clouds as a 
fundamental calibrator of stellar evolution and star-formation 
processes for understanding the stellar populations of distant 
galaxies. Effective exposure times are 977s in F275W, 1368s in F336W, 
4040s in F475W, 4042s in F814W, 699s in F110W, and 1796s in F160W, 
including short exposures to avoid saturation of bright sources. These 
depths will produce photon-limited images in the UV. Images will be 
crowding-limited in the optical and NIR, but will reach below the red 
clump at all radii. The images will reach the Nyquist sampling limit 
in F160W, F475W, and F814W.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UVI 11615&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Hunting for Optical Companions to Binary MSPs in Globular Clusters
&lt;/p&gt;&lt;p&gt;Here we present a proposal which exploits the renewed potential of HST 
after the Service Mission 4 for probing the population of binary 
Millisecond Pulsars (MSPs) in Globular Clusters. In particular we 
intend to: (1) extend the search for optical counterparts in Terzan 5, 
by pushing the performance of the WFC3 IR channel to sample the entire 
MS extension down to M=0.1 Mo; (2) perform a deep multi-band search of 
MSP companions with the WFC3, in 3 clusters (namely NGC6440, M28 and 
M5), where recent radio observations have found particularly 
interesting objects; (3) derive an accurate radial velocity (with 
STIS) of the puzzling optical companion COM6266B recently discovered 
by our group, to firmly assess its cluster membership. This program is 
the result of a large collaboration among the three major groups (lead 
by Freire, Ransom and Possenti) which are performing extensive MSP 
search in GCs in the radio bands, and our group which has a large 
experience in performing accurate stellar photometry in crowded 
environments. This collaboration has produced a number of outstanding 
discoveries. In fact, three of the 6 optical counterparts to binary 
MSP companions known to date in GCs have been discovered by our group. 
The observations here proposed would easily double/triple the existing 
sample of known MSP companions, allowing the first meaningful approach 
to the study of the formation, evolution and recycling process of 
pulsar in GCs. Moreover, since most of binary MSPs in GCs are thought 
to form via stellar interactions in the high density core regions, the 
determination of the nature of the companion and the incidence of this 
collisionally-induced population has a significant impact on our 
knowledge of the cluster dynamics. Even more interesting, the study of 
the optical companions to NSs in GCs allows one to derive tighter 
constraints (than those obtainable for NS binaries in the Galactic 
field) on the system properties. This has, in turn, an intrinsic 
importance for fundamental physics, since it offers the opportunity of 
measuring the mass of the NS and hence constraining the equation of 
state of matter at the nuclear equilibrium density.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UVIS 11907&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;UVIS Cycle 17 Contamination Monitor
&lt;/p&gt;&lt;p&gt;The UV throughput of WFC3 during Cycle 17 is monitored via weekly 
standard star observations in a subset of key filters covering 
200-600nm and F606W, F814W as controls on the red end. The data will 
provide a measure of throughput levels as a function of time and 
wavelength, allowing for detection of the presence of possible 
contaminants.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UVIS/IR 11909&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;UVIS Hot Pixel Anneal
&lt;/p&gt;&lt;p&gt;The on-orbit radiation environment of WFC3 will continually generate 
new hot pixels. This proposal performs the procedure required for 
repairing those hot pixels in the UVIS CCDs. During an anneal, the 
two-stage thermo-electric cooler (TEC) is turned off and the 
four-stage TEC is used as a heater to bring the UVIS CCDs up to ~20 
deg. C. As a result of the CCD warmup, a majority of the hot pixels 
will be fixed; previous instruments such as WFPC2 and ACS have seen 
repair rates of about 80%. Internal UVIS exposures are taken before 
and after each anneal, to allow an assessment of the procedure's 
effectiveness in WFC3, provide a check of bias, global dark current, 
and hot pixel levels, as well as support hysteresis (bowtie) 
monitoring and CDBS reference file generation. One IR dark is taken 
after each anneal, to provide a check of the IR detector.
&lt;/p&gt;

&lt;hr/&gt;
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  <entry>
    <title>Daily Report #5143</title>
    <link rel="alternate" href="http://www.aus-city.com/cgi-bin/dada/mail.cgi/archive/HST_REPORTS/20100723000503/"/>
    <id>tag:www.aus-city.com,2010-07-23:%2Fcgi-bin%2Fdada%2Fmail.cgi%2Farchive%2FHST_REPORTS%2F20100723000503%2F</id>
    
    <published>2010-07-23T00:05:03Z</published>
    <updated>2010-07-23T00:05:03Z</updated>
    <content type="html">

&lt;div class=WordSection1&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;HUBBLE SPACE
TELESCOPE - Continuing to Collect World Class Science &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;DAILY
REPORT #5143 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;PERIOD
COVERED: 5am July 21 - 5am July 22, 2010 (DOY 202/09:00z-203/09:00z) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;FLIGHT
OPERATIONS SUMMARY: &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Significant
Spacecraft Anomalies: (The following are preliminary reports&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;of
potential non-nominal performance that will be investigated.) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;HSTARS:
(None) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COMPLETED
OPS REQUEST: (None) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COMPLETED
OPS NOTES: (None) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&amp;#160;&amp;#160;&amp;#160;SCHEDULED&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
SUCCESSFUL&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160; &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;FGS
GSAcq&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;7&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
7&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;FGS
REAcq&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;9&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
9&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;OBAD with
Maneuver&amp;#160;&amp;#160;
3&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
3 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&amp;#160;&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;SIGNIFICANT
EVENTS: (None) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;OBSERVATIONS
SCHEDULED: &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;ACS/WFC
11996 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;CCD Daily
Monitor (Part 3) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;This program
comprises basic tests for measuring the read noise and dark&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;current of
the ACS WFC and for tracking the growth of hot pixels. The&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;recorded
frames are used to create bias and dark reference images for&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;science
data reduction and calibration. This program will be executed&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;four days
per week (Mon, Wed, Fri, Sun) for the duration of Cycle 17. To&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;facilitate
scheduling, this program is split into three proposals. This&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;proposal
covers 308 orbits (19.25 weeks) from 21 June 2010 to 1 November&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;2010. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;STIS/CC 11845
&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;CCD Dark
Monitor Part 2 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Monitor the
darks for the STIS CCD. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;STIS/CC
11847 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;CCD Bias
Monitor-Part 2 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Monitor the
bias in the 1x1, 1x2, 2x1, and 2x2 bin settings at gain=1,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;and 1x1 at
gain = 4, to build up high-S/N superbiases and track the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;evolution
of hot columns. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;STIS/CC/MA
11668 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Cosmo-chronometry
and Elemental Abundance Distribution of the Ancient&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Star
HE1523-0901 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;We propose
to obtain near-UV HST/STIS spectroscopy of the extremely&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;metal-poor,
highly r-process-enhanced halo star HE 1523-0901, in order&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;to produce
the most complete abundance distribution of the heaviest&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;stable
elements, including platinum, osmium, and lead. These HST&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;abundance
data will then be used to estimate the initial abundances of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the
long-lived radioactive elements thorium and uranium, and by&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;comparison
with their observed abundances, enable an accurate age&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;determination
of this ancient star. The use of radioactive chronometers&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;in stars
provides an independent lower limit on the age of the Galaxy,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;which can
be compared with alternative limits set by globular clusters&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;and by
analysis from WMAP. Our proposed observations of HE1523-0901 will&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;also
provide significant new information about the early chemical&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;history of
the Galaxy, specifically, the nature of the first generations&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;of stars
and the types of nucleosynthetic processes that occurred at the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;onset of
Galactic chemical evolution. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;STIS/MA1/MA2
11857 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;STIS Cycle
17 MAMA Dark Monitor &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;This
proposal monitors the behavior of the dark current in each of the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;MAMA
detectors. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;The basic
monitor takes two 1380s ACCUM darks each week with each&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;detector.
However, starting Oct 5, pairs are only included for weeks&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;that the
LRP has external MAMA observations planned. The weekly pairs of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;exposures
for each detector are linked so that they are taken at&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;opposite
ends of the same SAA free interval. This pairing of exposures&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;will make
it easier to separate long and short term temporal variability&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;from
temperature dependent changes. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;For both
detectors, additional blocks of exposures are taken once every&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;six months.
These are groups of five 1314s FUV-MAMA Time-Tag darks or&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;five 3x315s
NUV ACCUM darks distributed over a single SAA-free interval.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;This will
give more information on the brightness of the FUV MAMA dark&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;current as
a function of the amount of time that the HV has been on, and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;for the NUV
MAMA will give a better measure of the short term&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;temperature
dependence. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UV/ACS/WFC/IR
12058 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;A
Panchromatic Hubble Andromeda Treasury - I &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;We propose
to image the north east quadrant of M31 to deep limits in the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;UV,
optical, and near-IR. HST imaging should resolve the galaxy into&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;more than
100 million stars, all with common distances and foreground&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;extinctions.
UV through NIR stellar photometry (F275W, F336W with&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UVIS,
F475W and F814W with ACS/WFC, and F110W and F160W with&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/NIR)
will provide effective temperatures for a wide range of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;spectral
types, while simultaneously mapping M31's extinction. Our&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;central
science drivers are to: understand high-mass variations in the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;stellar IMF
as a function of SFR intensity and metallicity; capture the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;spatially-resolved
star formation history of M31; study a vast sample of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;stellar
clusters with a range of ages and metallicities. These are&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;central to
understanding stellar evolution and clustered star formation;&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;constraining
ISM energetics; and understanding the counterparts and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;environments
of transient objects (novae, SNe, variable stars, x-ray&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;sources, etc.).
As its legacy, this survey adds M31 to the Milky Way and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Magellanic
Clouds as a fundamental calibrator of stellar evolution and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;star-formation
processes for understanding the stellar populations of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;distant
galaxies. Effective exposure times are 977s in F275W, 1368s in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;F336W,
4040s in F475W, 4042s in F814W, 699s in F110W, and 1796s in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;F160W,
including short exposures to avoid saturation of bright sources.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;These
depths will produce photon-limited images in the UV. Images will&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;be
crowding-limited in the optical and NIR, but will reach below the red&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;clump at
all radii. The images will reach the Nyquist sampling limit in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;F160W,
F475W, and F814W. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UVI
11615 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Hunting for
Optical Companions to Binary MSPs in Globular Clusters &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Here we
present a proposal which exploits the renewed potential of HST&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;after the
Service Mission 4 for probing the population of binary&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Millisecond
Pulsars (MSPs) in Globular Clusters. In particular we intend&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;to: (1)
extend the search for optical counterparts in Terzan 5, by&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;pushing the
performance of the WFC3 IR channel to sample the entire MS&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;extension
down to M=0.1 Mo; (2) perform a deep multi-band search of MSP&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;companions
with the WFC3, in 3 clusters (namely NGC6440, M28 and M5),&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;where
recent radio observations have found particularly interesting&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;objects;
(3) derive an accurate radial velocity (with STIS) of the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;puzzling
optical companion COM6266B recently discovered by our group, to&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;firmly
assess its cluster membership. This program is the result of a&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;large
collaboration among the three major groups (lead by Freire, Ransom&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;and
Possenti) which are performing extensive MSP search in GCs in the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;radio
bands, and our group which has a large experience in performing&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;accurate stellar
photometry in crowded environments. This collaboration&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;has
produced a number of outstanding discoveries. In fact, three of the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;6 optical
counterparts to binary MSP companions known to date in GCs&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;have been
discovered by our group. The observations here proposed would&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;easily
double/triple the existing sample of known MSP companions,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;allowing
the first meaningful approach to the study of the formation,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;evolution
and recycling process of pulsar in GCs. Moreover, since most&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;of binary
MSPs in GCs are thought to form via stellar interactions in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the high
density core regions, the determination of the nature of the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;companion
and the incidence of this collisionally-induced population has&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;a
significant impact on our knowledge of the cluster dynamics. Even more&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;interesting,
the study of the optical companions to NSs in GCs allows&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;one to
derive tighter constraints (than those obtainable for NS binaries&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;in the
Galactic field) on the system properties. This has, in turn, an&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;intrinsic
importance for fundamental physics, since it offers the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;opportunity
of measuring the mass of the NS and hence constraining the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;equation of
state of matter at the nuclear equilibrium density. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UVIS
11907 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;UVIS Cycle
17 Contamination Monitor &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;The UV
throughput of WFC3 during Cycle 17 is monitored via weekly&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;standard
star observations in a subset of key filters covering 200-600nm&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;and F606W,
F814W as controls on the red end. The data will provide a&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;measure of
throughput levels as a function of time and wavelength,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;allowing
for detection of the presence of possible contaminants. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UVIS/IR
11909 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;UVIS Hot
Pixel Anneal &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;The
on-orbit radiation environment of WFC3 will continually generate new&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;hot pixels.
This proposal performs the procedure required for repairing&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;those hot pixels
in the UVIS CCDs. During an anneal, the two-stage&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;thermo-electric
cooler (TEC) is turned off and the four-stage TEC is&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;used as a
heater to bring the UVIS CCDs up to ~20 deg. C. As a result of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the CCD
warmup, a majority of the hot pixels will be fixed; previous&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;instruments
such as WFPC2 and ACS have seen repair rates of about 80%.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Internal
UVIS exposures are taken before and after each anneal, to allow&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;an
assessment of the procedure's effectiveness in WFC3, provide a check&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;of bias,
global dark current, and hot pixel levels, as well as support&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;hysteresis
(bowtie) monitoring and CDBS reference file generation. One&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;IR dark is
taken after each anneal, to provide a check of the IR&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;detector.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/p&gt;

&lt;p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto'&gt;&lt;span
style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;color:black'&gt;-&lt;/span&gt;&lt;span
style='font-size:10.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;color:black'&gt;Lynn&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&lt;/span&gt;&lt;b&gt;&lt;span style='font-family:&quot;Arial&quot;,&quot;sans-serif&quot;'&gt;&amp;#160;&amp;#160;&amp;#160;&lt;/span&gt;&lt;/b&gt;&lt;span
style='color:#1F497D'&gt;&lt;img width=123 height=99 id=&quot;Picture_x0020_1&quot;
src=&quot;cid:&amp;#105;&amp;#x6D;&amp;#x61;&amp;#103;&amp;#x65;&amp;#x30;&amp;#x30;&amp;#49;&amp;#46;&amp;#106;&amp;#112;&amp;#x67;&amp;#x40;&amp;#48;&amp;#x31;&amp;#67;&amp;#x42;&amp;#50;&amp;#57;&amp;#x38;&amp;#49;&amp;#x2E;&amp;#x42;&amp;#x34;&amp;#67;&amp;#x36;&amp;#x44;&amp;#50;&amp;#56;&amp;#48;&quot;
alt=&quot;cid:&amp;#105;&amp;#109;&amp;#97;&amp;#103;&amp;#x65;&amp;#48;&amp;#48;&amp;#49;&amp;#46;&amp;#x6A;&amp;#112;&amp;#x67;&amp;#x40;&amp;#48;&amp;#49;&amp;#67;&amp;#x41;&amp;#52;&amp;#55;&amp;#50;&amp;#x44;&amp;#46;&amp;#x43;&amp;#67;&amp;#65;&amp;#x36;&amp;#57;&amp;#x34;&amp;#68;&amp;#48;&quot;&gt;&lt;/span&gt;&lt;span style='font-size:10.0pt;
font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;color:black'&gt; &lt;/span&gt;&lt;span style='color:
black'&gt;&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto'&gt;&lt;span
style='font-size:10.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;color:black'&gt;NASA
office: 301-286-2876&lt;/span&gt;&lt;span style='color:black'&gt; &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto'&gt;&lt;span
style='font-size:10.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;color:black'&gt;__________________________________________________________&lt;br&gt;
Lynn F. Bassford&lt;br&gt;
&lt;/span&gt;&lt;span style='font-size:10.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;
color:blue'&gt;Hubble &lt;/span&gt;&lt;span style='font-size:10.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;
color:red'&gt;Space &lt;/span&gt;&lt;span style='font-size:10.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;
color:purple'&gt;Telescope&lt;br&gt;
&lt;/span&gt;&lt;span style='font-size:10.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;
color:black'&gt;CHAMP Mission Operations Manager&lt;/span&gt;&lt;span style='font-size:
10.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;color:purple'&gt;&lt;br&gt;
&lt;/span&gt;&lt;span style='font-size:10.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;
color:black'&gt;CHAMP Flight Operations Team Manager&lt;br&gt;
Lockheed Martin Mission Services (LMMS) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='color:black'&gt;&amp;#34;...Hubble is the most
significant science instrument of all time in terms of its
productivity...&amp;#34; &amp;#160;&amp;#160;&amp;#160;&amp;#160;Scott Altman @12:45pm 5/21/9
STS-125 Senate Subcommittee Hearing&lt;/span&gt;&lt;o:p&gt;&lt;/o:p&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/p&gt;

&lt;/div&gt;








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  <entry>
    <title>sci.astro.hubble - 2 new messages in 2 topics - digest</title>
    <link rel="alternate" href="http://www.aus-city.com/cgi-bin/dada/mail.cgi/archive/HST_REPORTS/20100722180502/"/>
    <id>tag:www.aus-city.com,2010-07-22:%2Fcgi-bin%2Fdada%2Fmail.cgi%2Farchive%2FHST_REPORTS%2F20100722180502%2F</id>
    
    <published>2010-07-22T18:05:02Z</published>
    <updated>2010-07-22T18:05:02Z</updated>
    <content type="html">
 
&lt;p&gt;sci.astro.hubble&lt;br/&gt;
&lt;a href=&quot;http://groups.google.com/group/sci.astro.hubble?hl=en&quot;&gt;http://groups.google.com/group/sci.astro.hubble?hl=en&lt;/a&gt;
&lt;/p&gt;&lt;p&gt;&lt;a href=&quot;mailto:&amp;#x73;&amp;#99;&amp;#x69;&amp;#46;&amp;#x61;&amp;#115;&amp;#116;&amp;#x72;&amp;#x6F;&amp;#46;&amp;#104;&amp;#117;&amp;#98;&amp;#x62;&amp;#108;&amp;#x65;&amp;#x40;&amp;#x67;&amp;#111;&amp;#x6F;&amp;#x67;&amp;#x6C;&amp;#x65;&amp;#103;&amp;#114;&amp;#x6F;&amp;#117;&amp;#x70;&amp;#115;&amp;#46;&amp;#x63;&amp;#111;&amp;#x6D;&quot;&gt;&amp;#x73;&amp;#99;&amp;#x69;&amp;#46;&amp;#x61;&amp;#115;&amp;#116;&amp;#x72;&amp;#x6F;&amp;#46;&amp;#104;&amp;#117;&amp;#98;&amp;#x62;&amp;#108;&amp;#x65;&amp;#x40;&amp;#x67;&amp;#111;&amp;#x6F;&amp;#x67;&amp;#x6C;&amp;#x65;&amp;#103;&amp;#114;&amp;#x6F;&amp;#117;&amp;#x70;&amp;#115;&amp;#46;&amp;#x63;&amp;#111;&amp;#x6D;&lt;/a&gt;
&lt;/p&gt;&lt;p&gt;Today's topics:
&lt;/p&gt;&lt;ul&gt;
  &lt;li&gt;Daily Report #5141 - 1 messages, 1 author
 &lt;a href=&quot;http://groups.google.com/group/sci.astro.hubble/t/081d819455fa1aa6?hl=en&quot;&gt;http://groups.google.com/group/sci.astro.hubble/t/081d819455fa1aa6?hl=en&lt;/a&gt;
  &lt;/li&gt;&lt;li&gt;Daily Report #5142 - 1 messages, 1 author
 &lt;a href=&quot;http://groups.google.com/group/sci.astro.hubble/t/5d7f4a3cadc34dd3?hl=en&quot;&gt;http://groups.google.com/group/sci.astro.hubble/t/5d7f4a3cadc34dd3?hl=en&lt;/a&gt;&lt;/li&gt;&lt;/ul&gt;
&lt;hr/&gt;
TOPIC: Daily Report #5141&lt;br/&gt;
&lt;a href=&quot;http://groups.google.com/group/sci.astro.hubble/t/081d819455fa1aa6?hl=en&quot;&gt;http://groups.google.com/group/sci.astro.hubble/t/081d819455fa1aa6?hl=en&lt;/a&gt;
&lt;hr/&gt;
&lt;p&gt;== 1 of 1 ==&lt;br/&gt;
Date: Tues, Jul 20 2010 8:46&amp;#194;&amp;#160;am 
From: &amp;#34;Bassford, Lynn&amp;#34;  
&lt;/p&gt;
&lt;p&gt;HUBBLE SPACE TELESCOPE - Continuing to Collect World Class Science
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;DAILY REPORT #5141&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;PERIOD COVERED: 5am July 19 - 5am July 20, 2010 (DOY 200/09:00z-201/09:00z)
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;FLIGHT OPERATIONS SUMMARY:&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Significant Spacecraft Anomalies: (The following are preliminary
reports of potential non-nominal performance that will be
investigated.)
&lt;/p&gt;&lt;dl&gt;
  &lt;dt&gt;HSTARS&lt;/dt&gt;
&lt;dd&gt;&lt;/dd&gt;&lt;/dl&gt;
&lt;p&gt;#12333 OBAD at 200/17:21:57z failed and GSAcq(1,2,1) at 200/17:26:57z
failed with search radius limit exceeded on FGS2
&lt;/p&gt;&lt;p&gt;Observations affected: Astrometry Proposal #12316
&lt;/p&gt;&lt;p&gt;From DOY 187:
&lt;/p&gt;&lt;p&gt;#12334 ReAcq(1,0,1) at 187/04:37:32z required two attempts for FL-DV
with scan step limit exceeded on FGS1
&lt;/p&gt;&lt;p&gt;COMPLETED OPS REQUEST: (None)
&lt;/p&gt;&lt;p&gt;COMPLETED OPS NOTES: (None)
&lt;/p&gt;&lt;pre&gt;
                             SCHEDULED      SUCCESSFUL
FGS GSAcq                     9               8
FGS REAcq                     7               7
OBAD with Maneuver            6               5&lt;/pre&gt;
&lt;p&gt;SIGNIFICANT EVENTS: (None)
&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;OBSERVATIONS SCHEDULED:&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;ACS/WFC 11996&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;CCD Daily Monitor (Part 3)
&lt;/p&gt;&lt;p&gt;This program comprises basic tests for measuring the read noise and
dark current of the ACS WFC and for tracking the growth of hot pixels.
The recorded frames are used to create bias and dark reference images
for science data reduction and calibration. This program will be
executed four days per week (Mon, Wed, Fri, Sun) for the duration of
Cycle 17. To facilitate scheduling, this program is split into three
proposals. This proposal covers 308 orbits (19.25 weeks) from 21 June
2010 to 1 November 2010.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;COS/FUV 11895&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;FUV Detector Dark Monitor
&lt;/p&gt;&lt;p&gt;Monitor the FUV detector dark rate by taking long science exposures
without illuminating the detector. The detector dark rate and spatial
distribution of counts will be compared to pre-launch and SMOV data in
order to verify the nominal operation of the detector. Variations of
count rate as a function of orbital position will be analyzed to find
dependence of dark rate on proximity to the SAA. Dependence of dark
rate as function of time will also be tracked.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;COS/NUV/FUV 11598&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;How Galaxies Acquire their Gas: A Map of Multiphase Accretion and
Feedback in Gaseous Galaxy Halos
&lt;/p&gt;&lt;p&gt;We propose to address two of the biggest open questions in galaxy
formation - how galaxies acquire their gas and how they return it to
the IGM - with a concentrated COS survey of diffuse multiphase gas in
the halos of SDSS galaxies at z = 0.15 - 0.35. Our chief science goal
is to establish a basic set of observational facts about the physical
state, metallicity, and kinematics of halo gas, including the sky
covering fraction of hot and cold material, the metallicity of infall
and outflow, and correlations with galaxy stellar mass, type, and
color - all as a function of impact parameter from 10 - 150 kpc.
Theory suggests that the bimodality of galaxy colors, the shape of the
luminosity function, and the mass-metallicity relation are all
influenced at a fundamental level by accretion and feedback, yet these
gas processes are poorly understood and cannot be predicted robustly
from first principles. We lack even a basic observational assessment
of the multiphase gaseous content of galaxy halos on 100 kpc scales,
and we do not know how these processes vary with galaxy properties.
This ignorance is presently one of the key impediments to
understanding galaxy formation in general. We propose to use the
high-resolution gratings G130M and G160M on the Cosmic Origins
Spectrograph to obtain sensitive column density measurements of a
comprehensive suite of multiphase ions in the spectra of 43 z &amp;#60; 1 QSOs
lying behind 43 galaxies selected from the Sloan Digital Sky Survey.
In aggregate, these sightlines will constitute a statistically sound
map of the physical state and metallicity of gaseous halos, and
subsets of the data with cuts on galaxy mass, color, and SFR will seek
out predicted variations of gas properties with galaxy properties. Our
interpretation of these data will be aided by state-of-the-art
hydrodynamic simulations of accretion and feedback, in turn providing
information to refine and test such models. We will also use Keck,
MMT, and Magellan (as needed) to obtain optical spectra of the QSOs to
measure cold gas with Mg II, and optical spectra of the galaxies to
measure SFRs and to look for outflows. In addition to our other
science goals, these observations will help place the Milky Way's
population of multiphase, accreting High Velocity Clouds (HVCs) into a
global context by identifying analogous structures around other
galaxies. Our program is designed to make optimal use of the unique
capabilities of COS to address our science goals and also generate a
rich dataset of other absorption-line systems.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;FGS 12316&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;HST/FGS Astrometric Search for Young Planets Around Beta Pic and AU
Mic
&lt;/p&gt;&lt;p&gt;AU Mic is a nearby Vega-type debris disk stars. Its disk system has
been spatially resolved in exquisite detail, predominantly via the ACS
coronagraph and WFPC-2 cameras onboard HST. These images exhibit a
wealth of morphological features which provide compelling indirect
evidence that AU Mic likely harbors short-period planetary body(ies).
We propose to use the superlative astrometric capabilities of HST/FGS
to directly detect these planets, hence provide the first direct
planet detection in a Vega-type system whose disk has been imaged at
high spatial resolution.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/CC 11845&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;CCD Dark Monitor Part 2
&lt;/p&gt;&lt;p&gt;Monitor the darks for the STIS CCD.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/CC 11847&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;CCD Bias Monitor-Part 2
&lt;/p&gt;&lt;p&gt;Monitor the bias in the 1x1, 1x2, 2x1, and 2x2 bin settings at gain=1,
and 1x1 at gain = 4, to build up high-S/N superbiases and track the
evolution of hot columns.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/CCD 11721&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Verifying the Utility of Type Ia Supernovae as Cosmological Probes:
Evolution and Dispersion in the Ultraviolet Spectra
&lt;/p&gt;&lt;p&gt;The study of distant type Ia supernova (SNe Ia) offers the most
practical and immediate discriminator between popular models of dark
energy. Yet fundamental questions remain over possible
redshift-dependent trends in their observed and intrinsic properties.
High-quality Keck spectroscopy of a representative sample of 36
intermediate redshift SNe Ia has revealed a surprising, and
unexplained, diversity in their rest-frame UV fluxes. One possible
explanation is hitherto undiscovered variations in the progenitor
metallicity. Unfortunately, this result cannot be compared to local UV
data as only two representative SNe Ia have been studied near maximum
light. Taking advantage of two new `rolling searches' and the
restoration of STIS, we propose a non-disruptive TOO campaign to
create an equivalent comparison local sample. This will allow us to
address possible evolution in the mean UV spectrum and its diversity,
an essential precursor to the study of SNe beyond z~1.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/CCD/MA2 11568&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;A SNAPSHOT Survey of the Local Interstellar Medium: New NUV
Observations of Stars with Archived FUV Observations
&lt;/p&gt;&lt;p&gt;We propose to obtain high-resolution STIS E230H SNAP observations of
MgII and FeII interstellar absorption lines toward stars within 100
parsecs that already have moderate or high-resolution far-UV (FUV),
900-1700 A, observations available in the MAST Archive. Fundamental
properties, such as temperature, turbulence, ionization, abundances,
and depletions of gas in the local interstellar medium (LISM) can be
measured by coupling such observations. Due to the wide spectral range
of STIS, observations to study nearby stars also contain important
data about the LISM embedded within their spectra. However, unlocking
this information from the intrinsically broad and often saturated FUV
absorption lines of low-mass ions, (DI, CII, NI, OI), requires first
understanding the kinematic structure of the gas along the line of
sight. This can be achieved with high resolution spectra of high-mass
ions, (FeII, MgII), which have narrow absorption lines, and can
resolve each individual velocity component (interstellar cloud). By
obtaining short (~10 minute) E230H observations of FeII and MgII, for
stars that already have moderate or high- resolution FUV spectra, we
can increase the sample of LISM measurements, and thereby expand our
knowledge of the physical properties of the gas in our galactic
neighborhood. STIS is the only instrument capable of obtaining the
required high resolution data now or in the foreseeable future.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/MA1/MA2 11857&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;STIS Cycle 17 MAMA Dark Monitor
&lt;/p&gt;&lt;p&gt;This proposal monitors the behavior of the dark current in each of the
MAMA detectors.
&lt;/p&gt;&lt;p&gt;The basic monitor takes two 1380s ACCUM darks each week with each
detector. However, starting Oct 5, pairs are only included for weeks
that the LRP has external MAMA observations planned. The weekly pairs
of exposures for each detector are linked so that they are taken at
opposite ends of the same SAA free interval. This pairing of exposures
will make it easier to separate long and short term temporal
variability from temperature dependent changes.
&lt;/p&gt;&lt;p&gt;For both detectors, additional blocks of exposures are taken once
every six months. These are groups of five 1314s FUV-MAMA Time-Tag
darks or five 3x315s NUV ACCUM darks distributed over a single
SAA-free interval. This will give more information on the brightness
of the FUV MAMA dark current as a function of the amount of time that
the HV has been on, and for the NUV MAMA will give a better measure of
the short term temperature dependence.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/ACS/UVIS/IR 11570&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Narrowing in on the Hubble Constant and Dark Energy
&lt;/p&gt;&lt;p&gt;A measurement of the Hubble constant to a precision of a few percent
would be a powerful aid to the investigation of the nature of dark
energy and a potent &amp;#34;end-to end&amp;#34; test of the present cosmological
model. In Cycle 15 we constructed a new streamlined distance ladder
utilizing high- quality type Ia supernova data and observations of
Cepheids with HST in the near-IR to minimize the dominant sources of
systematic uncertainty in past measurements of the Hubble constant and
reduce its total uncertainty to a little under 5%. Here we propose to
exploit this new route to reduce the remaining uncertainty by more
than 30%, translating into an equal reduction in the uncertainty of
the equation of state of dark energy. We propose three sets of
observations to reach this goal: a mosaic of NGC 4258 with WFC3 in
F160W to triple its sample of long period Cepheids, WFC3/F160W
observations of the 6 ideal SN Ia hosts to triple their samples of
Cepheids, and observations of NGC 5584 the host of a new SN Ia, SN
2007af, to discover and measure its Cepheids and begin expanding the
small set of SN Ia luminosity calibrations. These observations would
provide the bulk of a coordinated program aimed at making the
measurement of the Hubble constant one of the leading constraints on
dark energy.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/IR 11591&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Are Low-Luminosity Galaxies Responsible for Cosmic Reionization?
&lt;/p&gt;&lt;p&gt;Our group has demonstrated that massive clusters, acting as powerful
cosmic lenses, can constrain the abundance and properties of
low-luminosity star-forming sources beyond z~6; such sources are
thought to be responsible for ending cosmic reionization. The large
magnification possible in the critical regions of well-constrained
clusters brings sources into view that lie at or beyond the limits of
conventional exposures such as the UDF. We have shown that the
combination of HST and Spitzer is particularly effective in delivering
the physical properties of these distant sources, constraining their
mass, age and past star formation history. Indirectly, we therefore
gain a valuable glimpse to yet earlier epochs. Recognizing the result
(and limitations) of blank field surveys, we propose a systematic
search through 10 lensing clusters with ACS/F814W and
WFC3/[F110W+F160W] (in conjunction with existing deep IRAC data). Our
goal is to measure with great accuracy the luminosity function at z~7
over a range of at least 3 magnitude, based on the identification of
about 50 lensed galaxies at 6.5&amp;#60;z&amp;#60;8. Our survey will mitigate cosmic
variance and extend the search both to lower luminosities and, by
virtue of the WFC3/IRAC combination, to higher redshift. Thanks to the
lensing amplification spectroscopic follow-up will be possible and
make our findings the most robust prior to the era of JWST and the
ELTs.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/IR 11666&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Chilly Pairs: A Search for the Latest-type Brown Dwarf Binaries and
the Prototype Y Dwarf
&lt;/p&gt;&lt;p&gt;We propose to use HST/WFC3 to image a sample of 27 of the nearest (&amp;#60;
20 pc) and lowest luminosity T-type brown dwarfs in order to identify
and characterize new very low mass binary systems. Only 3 late-type T
dwarf binaries have been found to date, despite that fact that these
systems are critical benchmarks for evolutionary and atmospheric
models at the lowest masses. They are also the most likely systems to
harbor Y dwarf companions, an as yet unpopulated putative class of
very cold (T &amp;#60; 600 K) brown dwarfs. Our proposed program will more
than double the number of T5-T9 dwarfs imaged at high resolution, with
an anticipated yield of ~5 new binaries with initial characterization
of component spectral types. We will be able to probe separations
sufficient to identify systems suitable for astrometric orbit and
dynamical mass measurements. We also expect one of our discoveries to
contain the first Y-type brown dwarf. Our proposed program complements
and augments ongoing ground-based adaptive optics surveys and provides
pathway science for JWST.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/IR/S/C 11929&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;IR Dark Current Monitor
&lt;/p&gt;&lt;p&gt;Analyses of ground test data showed that dark current signals are more
reliably removed from science data using darks taken with the same
exposure sequences as the science data, than with a single dark
current image scaled by desired exposure time. Therefore, dark current
images must be collected using all sample sequences that will be used
in science observations. These observations will be used to monitor
changes in the dark current of the WFC3-IR channel on a day-to-day
basis, and to build calibration dark current ramps for each of the
sample sequences to be used by Gos in Cycle 17. For each sample
sequence/array size combination, a median ramp will be created and
delivered to the calibration database system (CDBS).
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UV/ACS/WFC 11636&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;First Resolved Imaging of Escaping Lyman Continuum
&lt;/p&gt;&lt;p&gt;The emission from star-forming galaxies appears to be responsible for
reionization of the universe at z &amp;#62; 6. However, the models that
attempt to describe the detailed impact of high-redshift galaxies on
the surrounding inter-galactic medium (IGM) are strongly dependent
upon several uncertain parameters. Perhaps the most uncertain is the
fraction of HI-ionizing photons produced by young stars that escape
into the IGM. Most attempts to measure this &amp;#34;escape fraction&amp;#34; have
produced null results. Recently, a small subset of z~3 Lyman Break
Galaxies (LBGs) has been found exhibiting large escape fractions. It
remains unclear however, what differentiates them from other LBGs.
Several models attempt to explain how such a large fraction of
ionizing continuum can escape through the HI and dust in the ISM (eg.
&amp;#34;chimneys&amp;#34; created by SNe winds, globular cluster formation, etc.),
each producing unique signatures which can be observed with resolved
imaging of the escaping Lyman continuum. To date, there are only six
LBGs with individual detections of escaping Lyman continuum at any
redshift. We propose a single deep, high resolution WFC3/UVIS image of
the ionizing continuum (F336W) and the rest-frame UV/optical
(F606W/F814W/F160W) of five of these six LBGs with large escape
fractions. These LBGs have a high surface density and large escape
fractions, and lie at the optimal redshift for Lyman continuum imaging
with UVIS filters, making our sample especially suitable for
follow-up. With these data we will discern the mechanisms responsible
for producing large escape fractions, and therefore gain insight into
the process of reionization.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UVIS 11905&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;WFC3 UVIS CCD Daily Monitor
&lt;/p&gt;&lt;p&gt;The behavior of the WFC3 UVIS CCD will be monitored daily with a set
of full-frame, four-amp bias and dark frames. A smaller set of 2Kx4K
subarray biases are acquired at less frequent intervals throughout the
cycle to support subarray science observations. The internals from
this proposal, along with those from the anneal procedure (Proposal
11909), will be used to generate the necessary superbias and superdark
reference files for the calibration pipeline (CDBS).
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UVIS 11908&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Cycle 17: UVIS Bowtie Monitor
&lt;/p&gt;&lt;p&gt;Ground testing revealed an intermittent hysteresis type effect in the
UVIS detector (both CCDs) at the level of ~1%, lasting hours to days.
Initially found via an unexpected bowtie-shaped feature in flatfield
ratios, subsequent lab tests on similar e2v devices have since shown
that it is also present as simply an overall offset across the entire
CCD, i.e., a QE offset without any discernable pattern. These lab
tests have further revealed that overexposing the detector to count
levels several times full well fills the traps and effectively
neutralizes the bowtie. Each visit in this proposal acquires a set of
three 3x3 binned internal flatfields: the first unsaturated image will
be used to detect any bowtie, the second, highly exposed image will
neutralize the bowtie if it is present, and the final image will allow
for verification that the bowtie is gone.
&lt;/p&gt;


&lt;hr/&gt;
TOPIC: Daily Report #5142&lt;br/&gt;
&lt;a href=&quot;http://groups.google.com/group/sci.astro.hubble/t/5d7f4a3cadc34dd3?hl=en&quot;&gt;http://groups.google.com/group/sci.astro.hubble/t/5d7f4a3cadc34dd3?hl=en&lt;/a&gt;
&lt;hr/&gt;
&lt;p&gt;== 1 of 1 ==&lt;br/&gt;
Date: Wed, Jul 21 2010 8:14&amp;#194;&amp;#160;am 
From: &amp;#34;Bassford, Lynn&amp;#34;  
&lt;/p&gt;
&lt;p&gt;HUBBLE SPACE TELESCOPE - Continuing to Collect World Class Science
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;DAILY REPORT #5142&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;PERIOD COVERED: 5am July 20 - 5am July 21, 2010 (DOY 201/09:00z-202/09:00z)
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;FLIGHT OPERATIONS SUMMARY:&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Significant Spacecraft Anomalies: (The following are preliminary
reports of potential non-nominal performance that will be
investigated.)
&lt;/p&gt;&lt;dl&gt;
  &lt;dt&gt;HSTARS&lt;/dt&gt;
&lt;dd&gt;&lt;/dd&gt;&lt;/dl&gt;
&lt;p&gt;From DOY 188:
&lt;/p&gt;&lt;p&gt;#12336 GSAcq(2,1,1) @188/14:11:27z required two attempts to achieve
CT-DV on FGS2. The acquisition was successful.
&lt;/p&gt;&lt;p&gt;COMPLETED OPS REQUEST: (None)
&lt;/p&gt;&lt;p&gt;COMPLETED OPS NOTES: (None)
&lt;/p&gt;&lt;pre&gt;
                             SCHEDULED      SUCCESSFUL
FGS GSAcq                     5                5
FGS REAcq                    11               11
OBAD with Maneuver            6                6&lt;/pre&gt;
&lt;p&gt;SIGNIFICANT EVENTS: (None)
&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;OBSERVATIONS SCHEDULED:&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;ACS/WFC3 11833&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Monitoring M31 for BHXNe
&lt;/p&gt;&lt;p&gt;During A01-8 we found ~20 Black Hole X-ray Novae (BHXNe) in M31 using
Chandra, and with HST follow-up have estimated orbital periods for 8
of these. Observations are underway with HST to attempt to estimate
additional periods. We propose to continue this program concentrating
our scarce HST resources on a single transient which exceeds 1e38
erg/s. Only uninterrupted monitoring can yield the duty cycles and
long-term light curves of BHXNe (and other variables) in M31. Our
GO+GTO programs will have accumulated 790ks (ACIS+HRC) near the M31
bulge by the end of AO9, and total Chandra exposure on M31 is now
940ks. By continuing our monitoring program through AO12 we will reach
~950ks on the bulge and &amp;#62;1Msec total Chandra M31 exposure.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;COS/FUV 11527&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;COS-GTO: An Absorption Study of Galactic Intermediate Velocity Clouds
Using Hot Stars in Globular Clusters
&lt;/p&gt;&lt;p&gt;We shall use UV bright hot post-AGB stars located within the globular
clusters of NGC 5139, NGC 6752, NGC 7078, NGC 6205, NGC 5272 and NGC
1904 to sample the UV absorption properties of the intervening
line-of-sight interstellar gas. Such sight-lines pass through several
intermediate velocity clouds (IVC?s) thought to be located within 5
kpc of our Galaxy, thus allowing the physical and chemical state of
this gas to be probed and compared with the properties of interstellar
gas located in the galactic disk. Elemental abundances of the IVC gas
shall be derived in order to determine a possible origin for these
in-falling galactic satellite cloud structures.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;COS/FUV 11686&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;The Cosmological Impact of AGN Outflows: Measuring Absolute Abundances
and Kinetic Luminosities
&lt;/p&gt;&lt;p&gt;AGN outflows are increasingly invoked as a major contributor to the
formation and evolution of supermassive black holes, their host
galaxies, the surrounding IGM, and cluster cooling flows. Our HST/COS
proposal will determine reliable absolute chemical abundances in six
AGN outflows, which influences several of the processes mentioned
above. To date there is only one such determination, done by our team
on Mrk 279 using 16 HST/STIS orbits and 100 ksec of FUSE time. The
advent of COS and its high sensitivity allows us to choose among
fainter objects at redshifts high enough to preclude the need for
FUSE. This will allow us to determine the absolute abundances for six
AGN (all fainter than Mrk 279) using only 40 HST COS orbits. This will
put abundances studies in AGN on a firm footing, an elusive goal for
the past four decades. In addition, prior FUSE observations of four of
these targets indicate that it is probable that the COS observations
will detect troughs from excited levels of C III. These will allow us
to measure the distances of the outflows and thereby determine their
kinetic luminosity, a major goal in AGN feedback research.
&lt;/p&gt;&lt;p&gt;We will use our state of the art column density extraction methods and
velocity-dependent photoionization models to determine the abundances
and kinetic luminosity. Previous AGN outflow projects suffered from
the constraints of deciding what science we could do using ONE of the
handful of bright targets that were observable. With COS we can choose
the best sample for our experiment. As an added bonus, most of the
spectral range of our targets has not been observed previously,
greatly increasing the discovery phase space.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/CC 11845&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;CCD Dark Monitor Part 2
&lt;/p&gt;&lt;p&gt;Monitor the darks for the STIS CCD.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/CC 11847&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;CCD Bias Monitor-Part 2
&lt;/p&gt;&lt;p&gt;Monitor the bias in the 1x1, 1x2, 2x1, and 2x2 bin settings at gain=1,
and 1x1 at gain = 4, to build up high-S/N superbiases and track the
evolution of hot columns.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/CCD 11721&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Verifying the Utility of Type Ia Supernovae as Cosmological Probes:
Evolution and Dispersion in the Ultraviolet Spectra
&lt;/p&gt;&lt;p&gt;The study of distant type Ia supernova (SNe Ia) offers the most
practical and immediate discriminator between popular models of dark
energy. Yet fundamental questions remain over possible
redshift-dependent trends in their observed and intrinsic properties.
High-quality Keck spectroscopy of a representative sample of 36
intermediate redshift SNe Ia has revealed a surprising, and
unexplained, diversity in their rest-frame UV fluxes. One possible
explanation is hitherto undiscovered variations in the progenitor
metallicity. Unfortunately, this result cannot be compared to local UV
data as only two representative SNe Ia have been studied near maximum
light. Taking advantage of two new `rolling searches' and the
restoration of STIS, we propose a non-disruptive TOO campaign to
create an equivalent comparison local sample. This will allow us to
address possible evolution in the mean UV spectrum and its diversity,
an essential precursor to the study of SNe beyond z~1.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/IR 11712&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Calibration of Surface Brightness Fluctuations for WFC3/IR
&lt;/p&gt;&lt;p&gt;We aim to characterize galaxy surface brightness fluctuations (SBF),
and calibrate the SBF distance method, in the F110W and F160W filters
of the Wide Field Camera 3 IR channel. Because of the very high
throughput of F110W and the good match of F160W to the standard H
band, we anticipate that both of these filters will be popular choices
for galaxy observations with WFC3/IR. The SBF signal is typically an
order of magnitude brighter in the near-IR than in the optical, and
the characteristics (sensitivity, FOV, cosmetics) of the WFC3/IR
channel will be enormously more efficient for SBF measurements than
previously available near-IR cameras. As a result, our proposed SBF
calibration will allow accurate distance derivation whenever an
early-type or bulge-dominated galaxy is observed out to a distance of
150 Mpc or more (i.e., out to the Hubble flow) in the calibrated
passbands. For individual galaxy observations, an accurate distance is
useful for establishing absolute luminosities, black hole masses,
linear sizes, etc. Eventually, once a large number of galaxies have
been observed across the sky with WFC3/IR, this SBF calibration will
enable accurate mapping of the total mass density distribution in the
local universe using the data available in the HST archive. The
proposed observations will have additional important scientific value;
in particular, we highlight their usefulness for understanding the
nature of multimodal globular cluster color distributions in giant
elliptical galaxies.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/IR/S/C 11929&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;IR Dark Current Monitor
&lt;/p&gt;&lt;p&gt;Analyses of ground test data showed that dark current signals are more
reliably removed from science data using darks taken with the same
exposure sequences as the science data, than with a single dark
current image scaled by desired exposure time. Therefore, dark current
images must be collected using all sample sequences that will be used
in science observations. These observations will be used to monitor
changes in the dark current of the WFC3-IR channel on a day-to-day
basis, and to build calibration dark current ramps for each of the
sample sequences to be used by Gos in Cycle 17. For each sample
sequence/array size combination, a median ramp will be created and
delivered to the calibration database system (CDBS).
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UVIS 11697&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Proper Motion Survey of Classical and SDSS Local Group Dwarf Galaxies
&lt;/p&gt;&lt;p&gt;Using the superior resolution of HST, we propose to continue our
proper motion survey of Galactic dwarf galaxies. The target galaxies
include one classical dwarf, Leo II, and six that were recently
identified in the Sloan Digital Sky Survey data: Bootes I, Canes
Venatici I, Canes Venatici II, Coma Berenices, Leo IV, and Ursa Major
II. We will observe a total of 16 fields, each centered on a
spectroscopically-confirmed QSO. Using QSOs as standards of rest in
measuring absolute proper motions has proven to be the most accurate
and most efficient method. HST is our only option to quickly determine
the space motions of the SDSS dwarfs because suitable ground-based
imaging is only a few years old and such data need several decades to
produce a proper motion. The two most distant galaxies in our sample
will require time baselines of four years to achieve our goal of a
30-50 km/s uncertainty in the tangential velocity; given this and the
finite lifetime of HST, it is imperative that first-epoch observations
be taken in this cycle. The SDSS dwarfs have dramatically lower
surface brightnesses and luminosities than the classical dwarfs.
Proper motions are crucial for determining orbits of the galaxies and
knowing the orbits will allow us to test theories for the formation
and evolution of these galaxies and, more generally, for the formation
of the Local Group.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UVIS 11905&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;WFC3 UVIS CCD Daily Monitor
&lt;/p&gt;&lt;p&gt;The behavior of the WFC3 UVIS CCD will be monitored daily with a set
of full-frame, four-amp bias and dark frames. A smaller set of 2Kx4K
subarray biases are acquired at less frequent intervals throughout the
cycle to support subarray science observations. The internals from
this proposal, along with those from the anneal procedure (Proposal
11909), will be used to generate the necessary superbias and superdark
reference files for the calibration pipeline (CDBS).
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UVIS/IR 11644&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;A Dynamical-Compositional Survey of the Kuiper Belt: A New Window Into
the Formation of the Outer Solar System
&lt;/p&gt;&lt;p&gt;The eight planets overwhelmingly dominate the solar system by mass,
but their small numbers, coupled with their stochastic pasts, make it
impossible to construct a unique formation history from the dynamical
or compositional characteristics of them alone. In contrast, the huge
numbers of small bodies scattered throughout and even beyond the
planets, while insignificant by mass, provide an almost unlimited
number of probes of the statistical conditions, history, and
interactions in the solar system. To date, attempts to understand the
formation and evolution of the Kuiper Belt have largely been dynamical
simulations where a hypothesized starting condition is evolved under
the gravitational influence of the early giant planets and an attempt
is made to reproduce the current observed populations. With little
compositional information known for the real Kuiper Belt, the test
particles in the simulation are free to have any formation location
and history as long as they end at the correct point. Allowing
compositional information to guide and constrain the formation,
thermal, and collisional histories of these objects would add an
entire new dimension to our understanding of the evolution of the
outer solar system. While ground based compositional studies have hit
their flux limits already with only a few objects sampled, we propose
to exploit the new capabilities of WFC3 to perform the first ever
large-scale dynamical-compositional study of Kuiper Belt Objects
(KBOs) and their progeny to study the chemical, dynamical, and
collisional history of the region of the giant planets. The
sensitivity of the WFC3 observations will allow us to go up to two
magnitudes deeper than our ground based studies, allowing us the
capability of optimally selecting a target list for a large survey
rather than simply taking the few objects that can be measured, as we
have had to do to date. We have carefully constructed a sample of 120
objects which provides both overall breadth, for a general
understanding of these objects, plus a large enough number of objects
in the individual dynamical subclass to allow detailed comparison
between and within these groups. These objects will likely define the
core Kuiper Belt compositional sample for years to come. While we have
many specific results anticipated to come from this survey, as with
any project where the field is rich, our current knowledge level is
low, and a new instrument suddenly appears which can exploit vastly
larger segments of the population, the potential for discovery -- both
anticipated and not -- is extraordinary.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UVIS/IR 11909&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;UVIS Hot Pixel Anneal
&lt;/p&gt;&lt;p&gt;The on-orbit radiation environment of WFC3 will continually generate
new hot pixels. This proposal performs the procedure required for
repairing those hot pixels in the UVIS CCDs. During an anneal, the
two-stage thermo-electric cooler (TEC) is turned off and the
four-stage TEC is used as a heater to bring the UVIS CCDs up to ~20
deg. C. As a result of the CCD warmup, a majority of the hot pixels
will be fixed; previous instruments such as WFPC2 and ACS have seen
repair rates of about 80%. Internal UVIS exposures are taken before
and after each anneal, to allow an assessment of the procedure's
effectiveness in WFC3, provide a check of bias, global dark current,
and hot pixel levels, as well as support hysteresis (bowtie)
monitoring and CDBS reference file generation. One IR dark is taken
after each anneal, to provide a check of the IR detector.
&lt;/p&gt;

&lt;hr/&gt;
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  <entry>
    <title>Daily Report #5142</title>
    <link rel="alternate" href="http://www.aus-city.com/cgi-bin/dada/mail.cgi/archive/HST_REPORTS/20100722020504/"/>
    <id>tag:www.aus-city.com,2010-07-22:%2Fcgi-bin%2Fdada%2Fmail.cgi%2Farchive%2FHST_REPORTS%2F20100722020504%2F</id>
    
    <published>2010-07-22T02:05:04Z</published>
    <updated>2010-07-22T02:05:04Z</updated>
    <content type="html">

&lt;div class=WordSection1&gt;

&lt;p class=MsoNormal&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;HUBBLE
SPACE TELESCOPE - Continuing to Collect World Class Science &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;DAILY
REPORT #5142 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;PERIOD
COVERED: 5am July 20 - 5am July 21, 2010 (DOY 201/09:00z-202/09:00z) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;FLIGHT
OPERATIONS SUMMARY: &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Significant
Spacecraft Anomalies: (The following are preliminary reports&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;of
potential non-nominal performance that will be investigated.) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;HSTARS: &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;From DOY
188:&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;#12336
GSAcq(2,1,1) @188/14:11:27z required two attempts to achieve&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&amp;#160;&amp;#160;&amp;#160; CT-DV on FGS2. The acquisition was successful. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COMPLETED
OPS REQUEST: (None) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COMPLETED
OPS NOTES: (None) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
SCHEDULED&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160; SUCCESSFUL &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;FGS
GSAcq&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
5&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
5&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;FGS
REAcq&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
11&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
11 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;OBAD with
Maneuver
&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;6&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
6&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;SIGNIFICANT
EVENTS: (None) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;OBSERVATIONS
SCHEDULED: &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;ACS/WFC3
11833 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Monitoring
M31 for BHXNe &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;During
A01-8 we found ~20 Black Hole X-ray Novae (BHXNe) in M31 using&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Chandra, and
with HST follow-up have estimated orbital periods for 8 of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;these.
Observations are underway with HST to attempt to estimate&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;additional
periods. We propose to continue this program concentrating&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;our scarce
HST resources on a single transient which exceeds 1e38 erg/s.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Only
uninterrupted monitoring can yield the duty cycles and long-term&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;light
curves of BHXNe (and other variables) in M31. Our GO+GTO programs&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;will have
accumulated 790ks (ACIS+HRC) near the M31 bulge by the end of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;AO9, and
total Chandra exposure on M31 is now 940ks. By continuing our&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;monitoring
program through AO12 we will reach ~950ks on the bulge and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&amp;#62;1Msec
total Chandra M31 exposure. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COS/FUV
11527 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COS-GTO: An
Absorption Study of Galactic Intermediate Velocity Clouds&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Using Hot
Stars in Globular Clusters &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;We shall
use UV bright hot post-AGB stars located within the globular&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;clusters of
NGC 5139, NGC 6752, NGC 7078, NGC 6205, NGC 5272 and NGC&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;1904 to
sample the UV absorption properties of the intervening&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;line-of-sight
interstellar gas. Such sight-lines pass through several&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;intermediate
velocity clouds (IVC?s) thought to be located within 5 kpc&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;of our
Galaxy, thus allowing the physical and chemical state of this gas&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;to be
probed and compared with the properties of interstellar gas&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;located in
the galactic disk. Elemental abundances of the IVC gas shall&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;be derived
in order to determine a possible origin for these in-falling&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;galactic
satellite cloud structures. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COS/FUV
11686 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;The Cosmological
Impact of AGN Outflows: Measuring Absolute Abundances&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;and Kinetic
Luminosities &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;AGN
outflows are increasingly invoked as a major contributor to the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;formation
and evolution of supermassive black holes, their host&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;galaxies,
the surrounding IGM, and cluster cooling flows. Our HST/COS&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;proposal
will determine reliable absolute chemical abundances in six AGN&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;outflows,
which influences several of the processes mentioned above. To&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;date there
is only one such determination, done by our team on Mrk 279&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;using 16
HST/STIS orbits and 100 ksec of FUSE time. The advent of COS&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;and its
high sensitivity allows us to choose among fainter objects at&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;redshifts
high enough to preclude the need for FUSE. This will allow us&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;to
determine the absolute abundances for six AGN (all fainter than Mrk&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;279) using
only 40 HST COS orbits. This will put abundances studies in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;AGN on a
firm footing, an elusive goal for the past four decades. In&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;addition,
prior FUSE observations of four of these targets indicate that&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;it is
probable that the COS observations will detect troughs from&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;excited
levels of C III. These will allow us to measure the distances of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the
outflows and thereby determine their kinetic luminosity, a major&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;goal in AGN
feedback research. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;We will use
our state of the art column density extraction methods and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;velocity-dependent
photoionization models to determine the abundances&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;and kinetic
luminosity. Previous AGN outflow projects suffered from the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;constraints
of deciding what science we could do using ONE of the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;handful of
bright targets that were observable. With COS we can choose&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the best
sample for our experiment. As an added bonus, most of the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;spectral
range of our targets has not been observed previously, greatly&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;increasing
the discovery phase space. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;STIS/CC
11845 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;CCD Dark
Monitor Part 2 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Monitor the
darks for the STIS CCD. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;STIS/CC
11847 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;CCD Bias
Monitor-Part 2 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Monitor the
bias in the 1x1, 1x2, 2x1, and 2x2 bin settings at gain=1,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;and 1x1 at
gain = 4, to build up high-S/N superbiases and track the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;evolution
of hot columns. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;STIS/CCD
11721 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Verifying
the Utility of Type Ia Supernovae as Cosmological Probes:&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Evolution
and Dispersion in the Ultraviolet Spectra &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;The study
of distant type Ia supernova (SNe Ia) offers the most&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;practical
and immediate discriminator between popular models of dark&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;energy. Yet
fundamental questions remain over possible&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;redshift-dependent
trends in their observed and intrinsic properties.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;High-quality
Keck spectroscopy of a representative sample of 36&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;intermediate
redshift SNe Ia has revealed a surprising, and unexplained,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;diversity
in their rest-frame UV fluxes. One possible explanation is&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;hitherto
undiscovered variations in the progenitor metallicity.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Unfortunately,
this result cannot be compared to local UV data as only&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;two
representative SNe Ia have been studied near maximum light. Taking&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;advantage
of two new `rolling searches' and the restoration of STIS, we&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;propose a
non-disruptive TOO campaign to create an equivalent comparison&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;local
sample. This will allow us to address possible evolution in the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;mean UV
spectrum and its diversity, an essential precursor to the study&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;of SNe
beyond z~1. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/IR
11712 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Calibration
of Surface Brightness Fluctuations for WFC3/IR &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;We aim to
characterize galaxy surface brightness fluctuations (SBF), and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;calibrate
the SBF distance method, in the F110W and F160W filters of the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Wide Field
Camera 3 IR channel. Because of the very high throughput of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;F110W and
the good match of F160W to the standard H band, we anticipate&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;that both
of these filters will be popular choices for galaxy&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;observations
with WFC3/IR. The SBF signal is typically an order of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;magnitude
brighter in the near-IR than in the optical, and the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;characteristics
(sensitivity, FOV, cosmetics) of the WFC3/IR channel&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;will be
enormously more efficient for SBF measurements than previously&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;available
near-IR cameras. As a result, our proposed SBF calibration&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;will allow
accurate distance derivation whenever an early-type or&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;bulge-dominated
galaxy is observed out to a distance of 150 Mpc or more&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;(i.e., out
to the Hubble flow) in the calibrated passbands. For&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;individual
galaxy observations, an accurate distance is useful for&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;establishing
absolute luminosities, black hole masses, linear sizes,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;etc.
Eventually, once a large number of galaxies have been observed&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;across the
sky with WFC3/IR, this SBF calibration will enable accurate&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;mapping of
the total mass density distribution in the local universe&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;using the
data available in the HST archive. The proposed observations&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;will have
additional important scientific value; in particular, we&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;highlight
their usefulness for understanding the nature of multimodal&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;globular
cluster color distributions in giant elliptical galaxies. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/IR/S/C
11929 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;IR Dark
Current Monitor &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Analyses of
ground test data showed that dark current signals are more&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;reliably
removed from science data using darks taken with the same&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;exposure
sequences as the science data, than with a single dark current&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;image
scaled by desired exposure time. Therefore, dark current images&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;must be
collected using all sample sequences that will be used in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;science
observations. These observations will be used to monitor changes&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;in the dark
current of the WFC3-IR channel on a day-to-day basis, and to&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;build
calibration dark current ramps for each of the sample sequences to&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;be used by
Gos in Cycle 17. For each sample sequence/array size&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;combination,
a median ramp will be created and delivered to the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;calibration
database system (CDBS). &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UVIS
11697 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Proper
Motion Survey of Classical and SDSS Local Group Dwarf Galaxies &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Using the
superior resolution of HST, we propose to continue our proper&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;motion survey
of Galactic dwarf galaxies. The target galaxies include&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;one
classical dwarf, Leo II, and six that were recently identified in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the Sloan
Digital Sky Survey data: Bootes I, Canes Venatici I, Canes&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Venatici
II, Coma Berenices, Leo IV, and Ursa Major II. We will observe&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;a total of
16 fields, each centered on a spectroscopically-confirmed&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;QSO. Using
QSOs as standards of rest in measuring absolute proper&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;motions has
proven to be the most accurate and most efficient method.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;HST is our
only option to quickly determine the space motions of the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;SDSS dwarfs
because suitable ground-based imaging is only a few years&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;old and
such data need several decades to produce a proper motion. The&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;two most
distant galaxies in our sample will require time baselines of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;four years
to achieve our goal of a 30-50 km/s uncertainty in the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;tangential
velocity; given this and the finite lifetime of HST, it is&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;imperative
that first-epoch observations be taken in this cycle. The&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;SDSS dwarfs
have dramatically lower surface brightnesses and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;luminosities
than the classical dwarfs. Proper motions are crucial for&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;determining
orbits of the galaxies and knowing the orbits will allow us&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;to test
theories for the formation and evolution of these galaxies and,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;more
generally, for the formation of the Local Group. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UVIS
11905 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3 UVIS
CCD Daily Monitor &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;The
behavior of the WFC3 UVIS CCD will be monitored daily with a set of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;full-frame,
four-amp bias and dark frames. A smaller set of 2Kx4K&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;subarray
biases are acquired at less frequent intervals throughout the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;cycle to
support subarray science observations. The internals from this&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;proposal,
along with those from the anneal procedure (Proposal 11909),&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;will be
used to generate the necessary superbias and superdark reference&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;files for the
calibration pipeline (CDBS). &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UVIS/IR
11644 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;A
Dynamical-Compositional Survey of the Kuiper Belt: A New Window Into&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the
Formation of the Outer Solar System &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;The eight
planets overwhelmingly dominate the solar system by mass, but&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;their small
numbers, coupled with their stochastic pasts, make it&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;impossible
to construct a unique formation history from the dynamical or&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;compositional
characteristics of them alone. In contrast, the huge&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;numbers of
small bodies scattered throughout and even beyond the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;planets,
while insignificant by mass, provide an almost unlimited number&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;of probes
of the statistical conditions, history, and interactions in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the solar
system. To date, attempts to understand the formation and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;evolution
of the Kuiper Belt have largely been dynamical simulations&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;where a
hypothesized starting condition is evolved under the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;gravitational
influence of the early giant planets and an attempt is&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;made to
reproduce the current observed populations. With little&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;compositional
information known for the real Kuiper Belt, the test&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;particles
in the simulation are free to have any formation location and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;history as
long as they end at the correct point. Allowing compositional&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;information
to guide and constrain the formation, thermal, and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;collisional
histories of these objects would add an entire new dimension&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;to our
understanding of the evolution of the outer solar system. While&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;ground
based compositional studies have hit their flux limits already&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;with only a
few objects sampled, we propose to exploit the new&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;capabilities
of WFC3 to perform the first ever large-scale&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;dynamical-compositional
study of Kuiper Belt Objects (KBOs) and their&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;progeny to
study the chemical, dynamical, and collisional history of the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;region of
the giant planets. The sensitivity of the WFC3 observations&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;will allow
us to go up to two magnitudes deeper than our ground based&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;studies,
allowing us the capability of optimally selecting a target list&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;for a large
survey rather than simply taking the few objects that can be&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;measured,
as we have had to do to date. We have carefully constructed a&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;sample of
120 objects which provides both overall breadth, for a general&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;understanding
of these objects, plus a large enough number of objects in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the individual
dynamical subclass to allow detailed comparison between&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;and within
these groups. These objects will likely define the core&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Kuiper Belt
compositional sample for years to come. While we have many&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;specific
results anticipated to come from this survey, as with any&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;project
where the field is rich, our current knowledge level is low, and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;a new
instrument suddenly appears which can exploit vastly larger&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;segments of
the population, the potential for discovery -- both&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;anticipated
and not -- is extraordinary. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;WFC3/UVIS/IR
11909 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;UVIS Hot
Pixel Anneal &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;The
on-orbit radiation environment of WFC3 will continually generate new&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;hot pixels.
This proposal performs the procedure required for repairing&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;those hot
pixels in the UVIS CCDs. During an anneal, the two-stage&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;thermo-electric
cooler (TEC) is turned off and the four-stage TEC is&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;used as a
heater to bring the UVIS CCDs up to ~20 deg. C. As a result of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the CCD
warmup, a majority of the hot pixels will be fixed; previous&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;instruments
such as WFPC2 and ACS have seen repair rates of about 80%.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Internal
UVIS exposures are taken before and after each anneal, to allow&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;an
assessment of the procedure's effectiveness in WFC3, provide a check&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;of bias,
global dark current, and hot pixel levels, as well as support&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;hysteresis
(bowtie) monitoring and CDBS reference file generation. One&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;IR dark is
taken after each anneal, to provide a check of the IR&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;detector.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/p&gt;

&lt;p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto'&gt;&lt;span
style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;color:black'&gt;-&lt;/span&gt;&lt;span
style='font-size:10.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;color:black'&gt;Lynn&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&lt;/span&gt;&lt;b&gt;&lt;span style='font-family:&quot;Arial&quot;,&quot;sans-serif&quot;'&gt;&amp;#160;&amp;#160;&amp;#160;&lt;/span&gt;&lt;/b&gt;&lt;span
style='color:#1F497D'&gt;&lt;img width=123 height=99 id=&quot;Picture_x0020_1&quot;
src=&quot;cid:&amp;#x69;&amp;#x6D;&amp;#x61;&amp;#103;&amp;#x65;&amp;#x30;&amp;#x30;&amp;#x31;&amp;#46;&amp;#106;&amp;#x70;&amp;#103;&amp;#x40;&amp;#48;&amp;#49;&amp;#67;&amp;#66;&amp;#50;&amp;#56;&amp;#67;&amp;#53;&amp;#x2E;&amp;#x32;&amp;#57;&amp;#66;&amp;#66;&amp;#50;&amp;#x34;&amp;#70;&amp;#48;&quot;
alt=&quot;cid:&amp;#x69;&amp;#109;&amp;#97;&amp;#103;&amp;#x65;&amp;#x30;&amp;#x30;&amp;#49;&amp;#x2E;&amp;#106;&amp;#x70;&amp;#x67;&amp;#x40;&amp;#48;&amp;#49;&amp;#x43;&amp;#65;&amp;#x34;&amp;#55;&amp;#x32;&amp;#x44;&amp;#x2E;&amp;#67;&amp;#67;&amp;#x41;&amp;#54;&amp;#57;&amp;#x34;&amp;#x44;&amp;#x30;&quot;&gt;&lt;/span&gt;&lt;span style='color:black'&gt;&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto'&gt;&lt;span
style='font-size:10.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;color:black'&gt;NASA
office: 301-286-2876&lt;/span&gt;&lt;span style='color:black'&gt;&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto'&gt;&lt;span
style='font-size:10.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;color:black'&gt;__________________________________________________________&lt;br&gt;
Lynn F. Bassford&lt;br&gt;
&lt;/span&gt;&lt;span style='font-size:10.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;
color:blue'&gt;Hubble &lt;/span&gt;&lt;span style='font-size:10.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;
color:red'&gt;Space &lt;/span&gt;&lt;span style='font-size:10.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;
color:purple'&gt;Telescope&lt;br&gt;
&lt;/span&gt;&lt;span style='font-size:10.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;
color:black'&gt;CHAMP Mission Operations Manager&lt;/span&gt;&lt;span style='font-size:
10.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;color:purple'&gt;&lt;br&gt;
&lt;/span&gt;&lt;span style='font-size:10.0pt;font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;;
color:black'&gt;CHAMP Flight Operations Team Manager&lt;br&gt;
Lockheed Martin Mission Services (LMMS) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='color:black'&gt;&amp;#34;...Hubble is the most significant
science instrument of all time in terms of its productivity...&amp;#34;
&amp;#160;&amp;#160;&amp;#160;&amp;#160;Scott Altman @12:45pm 5/21/9 STS-125 Senate
Subcommittee Hearing&lt;/span&gt;&lt;o:p&gt;&lt;/o:p&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/p&gt;

&lt;/div&gt;








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  <entry>
    <title>sci.astro.hubble - 3 new messages in 3 topics - digest</title>
    <link rel="alternate" href="http://www.aus-city.com/cgi-bin/dada/mail.cgi/archive/HST_REPORTS/20100721180503/"/>
    <id>tag:www.aus-city.com,2010-07-21:%2Fcgi-bin%2Fdada%2Fmail.cgi%2Farchive%2FHST_REPORTS%2F20100721180503%2F</id>
    
    <published>2010-07-21T18:05:03Z</published>
    <updated>2010-07-21T18:05:03Z</updated>
    <content type="html">
 
&lt;p&gt;sci.astro.hubble&lt;br/&gt;
&lt;a href=&quot;http://groups.google.com/group/sci.astro.hubble?hl=en&quot;&gt;http://groups.google.com/group/sci.astro.hubble?hl=en&lt;/a&gt;
&lt;/p&gt;&lt;p&gt;&lt;a href=&quot;mailto:&amp;#x73;&amp;#x63;&amp;#105;&amp;#x2E;&amp;#97;&amp;#115;&amp;#116;&amp;#x72;&amp;#x6F;&amp;#46;&amp;#104;&amp;#x75;&amp;#x62;&amp;#x62;&amp;#x6C;&amp;#101;&amp;#64;&amp;#103;&amp;#x6F;&amp;#x6F;&amp;#103;&amp;#108;&amp;#x65;&amp;#103;&amp;#x72;&amp;#111;&amp;#117;&amp;#112;&amp;#115;&amp;#46;&amp;#x63;&amp;#111;&amp;#x6D;&quot;&gt;&amp;#x73;&amp;#x63;&amp;#105;&amp;#x2E;&amp;#97;&amp;#115;&amp;#116;&amp;#x72;&amp;#x6F;&amp;#46;&amp;#104;&amp;#x75;&amp;#x62;&amp;#x62;&amp;#x6C;&amp;#101;&amp;#64;&amp;#103;&amp;#x6F;&amp;#x6F;&amp;#103;&amp;#108;&amp;#x65;&amp;#103;&amp;#x72;&amp;#111;&amp;#117;&amp;#112;&amp;#115;&amp;#46;&amp;#x63;&amp;#111;&amp;#x6D;&lt;/a&gt;
&lt;/p&gt;&lt;p&gt;Today's topics:
&lt;/p&gt;&lt;ul&gt;
  &lt;li&gt;Daily Report #5139 - 1 messages, 1 author
 &lt;a href=&quot;http://groups.google.com/group/sci.astro.hubble/t/b42485398f5b45b1?hl=en&quot;&gt;http://groups.google.com/group/sci.astro.hubble/t/b42485398f5b45b1?hl=en&lt;/a&gt;
  &lt;/li&gt;&lt;li&gt;Daily Report #5140 - 1 messages, 1 author
 &lt;a href=&quot;http://groups.google.com/group/sci.astro.hubble/t/c10e7789982b5429?hl=en&quot;&gt;http://groups.google.com/group/sci.astro.hubble/t/c10e7789982b5429?hl=en&lt;/a&gt;
  &lt;/li&gt;&lt;li&gt;Daily Report #5141 - 1 messages, 1 author
 &lt;a href=&quot;http://groups.google.com/group/sci.astro.hubble/t/081d819455fa1aa6?hl=en&quot;&gt;http://groups.google.com/group/sci.astro.hubble/t/081d819455fa1aa6?hl=en&lt;/a&gt;&lt;/li&gt;&lt;/ul&gt;
&lt;hr/&gt;
TOPIC: Daily Report #5139&lt;br/&gt;
&lt;a href=&quot;http://groups.google.com/group/sci.astro.hubble/t/b42485398f5b45b1?hl=en&quot;&gt;http://groups.google.com/group/sci.astro.hubble/t/b42485398f5b45b1?hl=en&lt;/a&gt;
&lt;hr/&gt;
&lt;p&gt;== 1 of 1 ==&lt;br/&gt;
Date: Fri, Jul 16 2010 9:03&amp;#194;&amp;#160;am 
From: &amp;#34;Bassford, Lynn&amp;#34;  
&lt;/p&gt;
&lt;p&gt;HUBBLE SPACE TELESCOPE - Continuing to Collect World Class Science
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;DAILY REPORT #5139&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;PERIOD COVERED: 5am July 15 - 5am July 16, 2010 (DOY 196/09:00z-197/09:00z)
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;FLIGHT OPERATIONS SUMMARY:&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Significant Spacecraft Anomalies: (The following are preliminary
reports of potential non-nominal performance that will be
investigated.)
&lt;/p&gt;&lt;p&gt;HSTARS: (None)
&lt;/p&gt;&lt;p&gt;COMPLETED OPS REQUEST: (None)
&lt;/p&gt;&lt;p&gt;COMPLETED OPS NOTES: (None)
&lt;/p&gt;&lt;pre&gt;
                                  SCHEDULED      SUCCESSFUL
FGS GSAcq                          9               9
FGS REAcq                          9               9
OBAD with Maneuver                 5               5&lt;/pre&gt;
&lt;p&gt;SIGNIFICANT EVENTS: (None)
&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;OBSERVATIONS SCHEDULED:&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;COS/FUV/STIS/CCD/MA1 11592&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Testing the Origin(s) of the Highly Ionized High-Velocity Clouds: A
Survey of Galactic Halo Stars at z&amp;#62;3 kpc
&lt;/p&gt;&lt;p&gt;Cosmological simulation predicts that highly ionized gas plays an
important role in the formation and evolution of galaxies and their
interplay with the intergalactic medium. The NASA HST and FUSE
missions have revealed high-velocity CIV and OVI absorption along
extragalactic sightlines through the Galactic halo. These highly
ionized high-velocity clouds (HVCs) could cover 85% of the sky and
have a detection rate higher than the HI HVCs. Two competing, equally
exciting, theories may explain the origin of these highly ionized
HVCs: 1) the &amp;#34;Galactic&amp;#34; theory, where the HVCs are the result of
feedback processes and trace the disk-halo mass exchange, perhaps
including the accretion of matter condensing from an extended corona;
2) the &amp;#34;Local Group&amp;#34; theory, where they are part of the local warm-hot
intergalactic medium, representing some of the missing baryonic matter
of the Universe. Only direct distance determinations can discriminate
between these models. Our group has found that some of these highly
ionized HVCs have a Galactic origin, based on STIS observations of one
star at z&amp;#60;5.3 kpc. We propose an HST FUV spectral survey to search for
and characterize the high velocity NV, CIV, and SiIV interstellar
absorption toward 24 stars at much larger distances than any previous
searches (4&amp;#60;d&amp;#60;21 kpc, 3&amp;#60;|z|&amp;#60;13 kpc). COS will provide atomic to highly
ionized species (e.g.,OI, CII, CIV, SiIV) that can be observed at
sufficient resolution (R~22, 000) to not only detect these highly
ionized HVCs but also to model their properties and understand their
physics and origins. This survey is only possible because of the high
sensitivity of COS in the FUV spectral range.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/CC 11845&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;CCD Dark Monitor Part 2
&lt;/p&gt;&lt;p&gt;Monitor the darks for the STIS CCD.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/CC 11847&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;CCD Bias Monitor-Part 2
&lt;/p&gt;&lt;p&gt;Monitor the bias in the 1x1, 1x2, 2x1, and 2x2 bin settings at gain=1,
and 1x1 at gain = 4, to build up high-S/N superbiases and track the
evolution of hot columns.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/CCD 11999&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;JWST Calibration from a Consistent Absolute Calibration of Spitzer &amp;
Hubble
&lt;/p&gt;&lt;p&gt;Recently, Gordon, Bohlin, et al. submitted a successful Spitzer
proposal for cross calibration of HST and Spitzer. The
cross-calibration targets are stars in three categories: WDs, A-stars,
and G-stars. Traditionally, IR flux standards are extrapolations of
stellar models that are tied to absolute fluxes at shorter
wavelengths. HST absolute flux standards are among the best available
with a solid basis that uses pure hydrogen models of hot WD stars for
the SED slopes and is tied to Vega at 5556A via precise Landolt V-band
photometry. Consistently matching models to our three categories of
HST observations along with Spitzer photometry and the few existing
absolute IR flux determinations will provide a solid basis for JWST
flux calibration over its 0.8-30micron range. The goal of this
proposal is to complete the HST observations of the set of HST/Spitzer
cross-calibration stars. Using a variety of standard stars with three
different spectral types will ensure that the final calibration is not
significantly affected by systematic uncertainties.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/IR 11666&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Chilly Pairs: A Search for the Latest-type Brown Dwarf Binaries and
the Prototype Y Dwarf
&lt;/p&gt;&lt;p&gt;We propose to use HST/WFC3 to image a sample of 27 of the nearest (&amp;#60;
20 pc) and lowest luminosity T-type brown dwarfs in order to identify
and characterize new very low mass binary systems. Only 3 late-type T
dwarf binaries have been found to date, despite that fact that these
systems are critical benchmarks for evolutionary and atmospheric
models at the lowest masses. They are also the most likely systems to
harbor Y dwarf companions, an as yet unpopulated putative class of
very cold (T &amp;#60; 600 K) brown dwarfs. Our proposed program will more
than double the number of T5-T9 dwarfs imaged at high resolution, with
an anticipated yield of ~5 new binaries with initial characterization
of component spectral types. We will be able to probe separations
sufficient to identify systems suitable for astrometric orbit and
dynamical mass measurements. We also expect one of our discoveries to
contain the first Y-type brown dwarf. Our proposed program complements
and augments ongoing ground-based adaptive optics surveys and provides
pathway science for JWST.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/IR/S/C 11929&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;IR Dark Current Monitor
&lt;/p&gt;&lt;p&gt;Analyses of ground test data showed that dark current signals are more
reliably removed from science data using darks taken with the same
exposure sequences as the science data, than with a single dark
current image scaled by desired exposure time. Therefore, dark current
images must be collected using all sample sequences that will be used
in science observations. These observations will be used to monitor
changes in the dark current of the WFC3-IR channel on a day-to-day
basis, and to build calibration dark current ramps for each of the
sample sequences to be used by Gos in Cycle 17. For each sample
sequence/array size combination, a median ramp will be created and
delivered to the calibration database system (CDBS).
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UV 11605&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Obtaining the Missing Links in the Test of Very Low Mass Evolutionary
Models with HST
&lt;/p&gt;&lt;p&gt;We are proposing for spatially resolved ACS+HRC observations of 11
very low mass binaries spanning late-M, L and T spectral types in
order to obtain precise effective temperature measurements for each
component. All of our targets are part of a program in which we are
measuring dynamical masses of very low-mass binaries to an
unprecedented precision of 10% (or better). However, without precise
temperature measurements, the full scientific value of these mass
measurements cannot be realized. Together, mass and temperature
measurements will allow us to distinguish between brown dwarf
evolutionary models that make different assumptions about the interior
and atmospheric structure of these ultra-cool objects. While dynamical
masses can be obtained from the ground in the near-IR, obtaining
precise temperatures require access to optical data which, for these
sub-arcsecond binaries, can only be obtained from space with Hubble.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UV/ACS/WFC/IR 12057&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;A Panchromatic Hubble Andromeda Treasury - I
&lt;/p&gt;&lt;p&gt;We propose to image the north east quadrant of M31 to deep limits in
the UV, optical, and near-IR. HST imaging should resolve the galaxy
into more than 100 million stars, all with common distances and
foreground extinctions. UV through NIR stellar photometry (F275W,
F336W with WFC3/UVIS, F475W and F814W with ACS/WFC, and F110W and
F160W with WFC3/NIR) will provide effective temperatures for a wide
range of spectral types, while simultaneously mapping M31's
extinction. Our central science drivers are to: understand high-mass
variations in the stellar IMF as a function of SFR intensity and
metallicity; capture the spatially-resolved star formation history of
M31; study a vast sample of stellar clusters with a range of ages and
metallicities. These are central to understanding stellar evolution
and clustered star formation; constraining ISM energetics; and
understanding the counterparts and environments of transient objects
(novae, SNe, variable stars, x-ray sources, etc.). As its legacy, this
survey adds M31 to the Milky Way and Magellanic Clouds as a
fundamental calibrator of stellar evolution and star-formation
processes for understanding the stellar populations of distant
galaxies. Effective exposure times are 977s in F275W, 1368s in F336W,
4040s in F475W, 4042s in F814W, 699s in F110W, and 1796s in F160W,
including short exposures to avoid saturation of bright sources. These
depths will produce photon-limited images in the UV. Images will be
crowding-limited in the optical and NIR, but will reach below the red
clump at all radii. The images will reach the Nyquist sampling limit
in F160W, F475W, and F814W.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UVIS 11577&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Opening New Windows on the Antennae with WFC3
&lt;/p&gt;&lt;p&gt;We propose to use WFC3 to provide key observations of young star
clusters in &amp;#34;The Antennae&amp;#34; (NGC4038/39). Of prime importance is the
WFC3's ability to push the limiting UV magnitude FIVE mag deeper than
our previous WFPC2 observations. This corresponds to pushing the
limiting cluster mass from ~10**5 to ~10**3 solar masses for cluster
ages ~10**8 yrs. In addition, the much wider field of view of the WFC3
IR channel will allow us to map out both colliding disks rather than
just the Overlap Region between them. This will be especially
important for finding the youngest clusters that are still embedded in
their placental cocoons. The extensive set of narrow-band filters will
provide an effective means for determining the properties of shocks,
which are believed to be a primary triggering mechanism for star
formation. We will also use ACS in parallel with WFC3 to observe
portions of both the northern and southern tails at no additional
orbital cost. Finally, one additional primary WFC3 orbit will be used
to supplement exisiting HST observations of the star-forming &amp;#34;dwarf&amp;#34;
galaxy at the end of the southern tail. Hence, when completed we will
have full UBVI + H_alpha coverage (or more for the main galaxy) of
four different environments in the Antennae. In conjunction with the
extensive multi- wavelength database we have collected (both HST and
ground based) these observations will provide answers to fundamental
questions such as: How do these clusters form and evolve? How is star
formation triggered? How do star clusters affect the local and global
ISM, and the evolution of the galaxy as a whole? The Antennae galaxies
are the nearest example of a major disk--disk merger, and hence may
represent our best chance for understanding how mergers form
tremendous numbers of clusters and stars, both in the local universe
and during galaxy assembly at high redshift.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UVIS 11594&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;A WFC3 Grism Survey for Lyman Limit Absorption at z=2
&lt;/p&gt;&lt;p&gt;We propose to conduct a spectroscopic survey of Lyman limit absorbers
at redshifts 1.8 &amp;#60; z &amp;#60; 2.5, using WFC3 and the G280 grism. This
proposal intends to complete an approved Cycle 15 SNAP program
(10878), which was cut short due to the ACS failure. We have selected
64 quasars at 2.3 &amp;#60; z &amp;#60; 2.6 from the Sloan Digital Sky Survey
Spectroscopic Quasar Sample, for which no BAL signature is found at
the QSO redshift and no strong metal absorption lines are present at z
&lt;span class=&quot;quoted_reply&quot;&gt;&amp;#62; 2.3 along the lines of sight. The survey has three main&lt;/span&gt;
observational goals. First, we will determine the redshift frequency
dn/dz of the LLS over the column density range 16.0 &amp;#60; log(NHI) &amp;#60; 20.3
cm^-2. Second, we will measure the column density frequency
distribution f(N) for the partial Lyman limit systems (PLLS) over the
column density range 16.0 &amp;#60; log(NHI) &amp;#60; 17.5 cm^-2. Third, we will
identify those sightlines which could provide a measurement of the
primordial D/H ratio. By carrying out this survey, we can also help
place meaningful constraints on two key quantities of cosmological
relevance. First, we will estimate the amount of metals in the LLS
using the f(N), and ground based observations of metal line
transitions. Second, by determining f(N) of the PLLS, we can constrain
the amplitude of the ionizing UV background at z~2 to a greater
precision. This survey is ideal for a snapshot observing program,
because the on-object integration times are all well below 30 minutes,
and follow-up observations from the ground require minimal telescope
time due to the QSO sample being bright.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UVIS 11661&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;The Black Hole Mass - Bulge Luminosity Relationship for the Nearest
Reverberation-Mapped AGNs
&lt;/p&gt;&lt;p&gt;We propose to obtain WFC3 host galaxy images of the eight nearest AGNs
with masses from reverberation mapping, and one star as a PSF model.
These images will allow us to determine with unprecedented accuracy
the bulge luminosities of the host galaxies, a goal which is not
achievable from the ground due to the blurring of the very bright PSF
component under typical, and even very good, seeing conditions.
High-resolution ACS images of the host galaxies of more luminous AGNs
reveal that the black hole mass-bulge luminosity and black hole
mass-bulge mass relationships for AGNs are not well constrained and
arise from what appear to be fundamentally flawed data sets. With the
addition of the images proposed here to our current sample of ACS
images, we will be able to extend our determinations of the black hole
mass- bulge luminosity and black hole mass-bulge mass relationships
for AGNs by an order of magnitude and test our preliminary results for
these fundamentally important relationships against those previously
determined for quiescent galaxies.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UVIS 11905&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;WFC3 UVIS CCD Daily Monitor
&lt;/p&gt;&lt;p&gt;The behavior of the WFC3 UVIS CCD will be monitored daily with a set
of full-frame, four-amp bias and dark frames. A smaller set of 2Kx4K
subarray biases are acquired at less frequent intervals throughout the
cycle to support subarray science observations. The internals from
this proposal, along with those from the anneal procedure (Proposal
11909), will be used to generate the necessary superbias and superdark
reference files for the calibration pipeline (CDBS).
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UVIS 11908&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Cycle 17: UVIS Bowtie Monitor
&lt;/p&gt;&lt;p&gt;Ground testing revealed an intermittent hysteresis type effect in the
UVIS detector (both CCDs) at the level of ~1%, lasting hours to days.
Initially found via an unexpected bowtie-shaped feature in flatfield
ratios, subsequent lab tests on similar e2v devices have since shown
that it is also present as simply an overall offset across the entire
CCD, i.e., a QE offset without any discernable pattern. These lab
tests have further revealed that overexposing the detector to count
levels several times full well fills the traps and effectively
neutralizes the bowtie. Each visit in this proposal acquires a set of
three 3x3 binned internal flatfields: the first unsaturated image will
be used to detect any bowtie, the second, highly exposed image will
neutralize the bowtie if it is present, and the final image will allow
for verification that the bowtie is gone.
&lt;/p&gt;


&lt;hr/&gt;
TOPIC: Daily Report #5140&lt;br/&gt;
&lt;a href=&quot;http://groups.google.com/group/sci.astro.hubble/t/c10e7789982b5429?hl=en&quot;&gt;http://groups.google.com/group/sci.astro.hubble/t/c10e7789982b5429?hl=en&lt;/a&gt;
&lt;hr/&gt;
&lt;p&gt;== 1 of 1 ==&lt;br/&gt;
Date: Mon, Jul 19 2010 7:19&amp;#194;&amp;#160;am 
From: &amp;#34;Bassford, Lynn&amp;#34;  
&lt;/p&gt;
&lt;p&gt;HUBBLE SPACE TELESCOPE - Continuing to Collect World Class Science
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;DAILY REPORT #5140&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;PERIOD COVERED: 5am July 16 - 5am July 19, 2010 (DOY 197/09:00z-200/09:00z)
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;FLIGHT OPERATIONS SUMMARY:&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Significant Spacecraft Anomalies: (The following are preliminary
reports of potential non-nominal performance that will be
investigated.)
&lt;/p&gt;&lt;dl&gt;
  &lt;dt&gt;HSTARS&lt;/dt&gt;
&lt;dd&gt;&lt;/dd&gt;&lt;/dl&gt;
&lt;p&gt;#12330 REAcq(1,2,1) @197/19:28z and 21:04z failed to RGA, Scan Step
Limit on FGS1
&lt;/p&gt;&lt;p&gt;Observations affected: COS #54-59 and ACS #120-126 Proposal #11658
&lt;/p&gt;&lt;p&gt;COMPLETED OPS REQUEST: (None)
&lt;/p&gt;&lt;p&gt;COMPLETED OPS NOTES: (None)
&lt;/p&gt;&lt;pre&gt;
                            SCHEDULED      SUCCESSFUL
GSAcq                      25              25
FGS REAcq                  24              22
OBAD with Maneuver         20              20&lt;/pre&gt;
&lt;p&gt;SIGNIFICANT EVENTS: (None)
&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;OBSERVATIONS SCHEDULED:&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UV/ACS/WFC/IR 12057&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;A Panchromatic Hubble Andromeda Treasury - I
&lt;/p&gt;&lt;p&gt;We propose to image the north east quadrant of M31 to deep limits in
the UV, optical, and near-IR. HST imaging should resolve the galaxy
into more than 100 million stars, all with common distances and
foreground extinctions. UV through NIR stellar photometry (F275W,
F336W with WFC3/UVIS, F475W and F814W with ACS/WFC, and F110W and
F160W with WFC3/NIR) will provide effective temperatures for a wide
range of spectral types, while simultaneously mapping M31's
extinction. Our central science drivers are to: understand high-mass
variations in the stellar IMF as a function of SFR intensity and
metallicity; capture the spatially-resolved star formation history of
M31; study a vast sample of stellar clusters with a range of ages and
metallicities. These are central to understanding stellar evolution
and clustered star formation; constraining ISM energetics; and
understanding the counterparts and environments of transient objects
(novae, SNe, variable stars, x-ray sources, etc.). As its legacy, this
survey adds M31 to the Milky Way and Magellanic Clouds as a
fundamental calibrator of stellar evolution and star-formation
processes for understanding the stellar populations of distant
galaxies. Effective exposure times are 977s in F275W, 1368s in F336W,
4040s in F475W, 4042s in F814W, 699s in F110W, and 1796s in F160W,
including short exposures to avoid saturation of bright sources. These
depths will produce photon-limited images in the UV. Images will be
crowding-limited in the optical and NIR, but will reach below the red
clump at all radii. The images will reach the Nyquist sampling limit
in F160W, F475W, and F814W.
&lt;/p&gt;&lt;p&gt;S/C 12046
&lt;/p&gt;&lt;p&gt;COS FUV DCE Memory Dump
&lt;/p&gt;&lt;p&gt;Whenever the FUV detector high voltage is on, count rate and current
draw information is collected, monitored, and saved to DCE memory.
Every 10 msec the detector samples the currents from the HV power
supplies (HVIA, HVIB) and the AUX power supply (AUXI). The last 1000
samples are saved in memory, along with a histogram of the number of
occurrences of each current value.
&lt;/p&gt;&lt;p&gt;In the case of a HV transient (known as a &amp;#34;crackle&amp;#34; on FUSE), where
one of these currents exceeds a preset threshold for a persistence
time, the HV will shut down, and the DCE memory will be dumped and
examined as part of the recovery procedure. However, if the current
exceeds the threshold for less than the persistence time (a
&amp;#34;mini-crackle&amp;#34; in FUSE parlance), there is no way to know without
dumping DCE memory. By dumping and examining the histograms regularly,
we will be able to monitor any changes in the rate of &amp;#34;mini-crackles&amp;#34;
and thus learn something about the state of the detector.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;ACS/WFC 11996&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;CCD Daily Monitor (Part 3)
&lt;/p&gt;&lt;p&gt;This program comprises basic tests for measuring the read noise and
dark current of the ACS WFC and for tracking the growth of hot pixels.
The recorded frames are used to create bias and dark reference images
for science data reduction and calibration. This program will be
executed four days per week (Mon, Wed, Fri, Sun) for the duration of
Cycle 17. To facilitate scheduling, this program is split into three
proposals. This proposal covers 308 orbits (19.25 weeks) from 21 June
2010 to 1 November 2010.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/IR/S/C 11929&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;IR Dark Current Monitor
&lt;/p&gt;&lt;p&gt;Analyses of ground test data showed that dark current signals are more
reliably removed from science data using darks taken with the same
exposure sequences as the science data, than with a single dark
current image scaled by desired exposure time. Therefore, dark current
images must be collected using all sample sequences that will be used
in science observations. These observations will be used to monitor
changes in the dark current of the WFC3-IR channel on a day-to-day
basis, and to build calibration dark current ramps for each of the
sample sequences to be used by Gos in Cycle 17. For each sample
sequence/array size combination, a median ramp will be created and
delivered to the calibration database system (CDBS).
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UVIS 11908&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Cycle 17: UVIS Bowtie Monitor
&lt;/p&gt;&lt;p&gt;Ground testing revealed an intermittent hysteresis type effect in the
UVIS detector (both CCDs) at the level of ~1%, lasting hours to days.
Initially found via an unexpected bowtie-shaped feature in flatfield
ratios, subsequent lab tests on similar e2v devices have since shown
that it is also present as simply an overall offset across the entire
CCD, i.e., a QE offset without any discernable pattern. These lab
tests have further revealed that overexposing the detector to count
levels several times full well fills the traps and effectively
neutralizes the bowtie. Each visit in this proposal acquires a set of
three 3x3 binned internal flatfields: the first unsaturated image will
be used to detect any bowtie, the second, highly exposed image will
neutralize the bowtie if it is present, and the final image will allow
for verification that the bowtie is gone.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UVIS 11907&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;UVIS Cycle 17 Contamination Monitor
&lt;/p&gt;&lt;p&gt;The UV throughput of WFC3 during Cycle 17 is monitored via weekly
standard star observations in a subset of key filters covering
200-600nm and F606W, F814W as controls on the red end. The data will
provide a measure of throughput levels as a function of time and
wavelength, allowing for detection of the presence of possible
contaminants.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UVIS 11905&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;WFC3 UVIS CCD Daily Monitor
&lt;/p&gt;&lt;p&gt;The behavior of the WFC3 UVIS CCD will be monitored daily with a set
of full-frame, four-amp bias and dark frames. A smaller set of 2Kx4K
subarray biases are acquired at less frequent intervals throughout the
cycle to support subarray science observations. The internals from
this proposal, along with those from the anneal procedure (Proposal
11909), will be used to generate the necessary superbias and superdark
reference files for the calibration pipeline (CDBS).
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/MA1/MA2 11857&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;STIS Cycle 17 MAMA Dark Monitor
&lt;/p&gt;&lt;p&gt;This proposal monitors the behavior of the dark current in each of the
MAMA detectors.
&lt;/p&gt;&lt;p&gt;The basic monitor takes two 1380s ACCUM darks each week with each
detector. However, starting Oct 5, pairs are only included for weeks
that the LRP has external MAMA observations planned. The weekly pairs
of exposures for each detector are linked so that they are taken at
opposite ends of the same SAA free interval. This pairing of exposures
will make it easier to separate long and short term temporal
variability from temperature dependent changes.
&lt;/p&gt;&lt;p&gt;For both detectors, additional blocks of exposures are taken once
every six months. These are groups of five 1314s FUV-MAMA Time-Tag
darks or five 3x315s NUV ACCUM darks distributed over a single
SAA-free interval. This will give more information on the brightness
of the FUV MAMA dark current as a function of the amount of time that
the HV has been on, and for the NUV MAMA will give a better measure of
the short term temperature dependence.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/CC 11847&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;CCD Bias Monitor-Part 2
&lt;/p&gt;&lt;p&gt;Monitor the bias in the 1x1, 1x2, 2x1, and 2x2 bin settings at gain=1,
and 1x1 at gain = 4, to build up high-S/N superbiases and track the
evolution of hot columns.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/CC 11845&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;CCD Dark Monitor Part 2
&lt;/p&gt;&lt;p&gt;Monitor the darks for the STIS CCD.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/IR 11838&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Completing a Flux-limited Survey for X-ray Emission from Radio Jets
&lt;/p&gt;&lt;p&gt;We will measure the changing flow speeds, magnetic fields, and energy
fluxes in well-resolved quasar jets found in our short-exposure
Chandra survey by combining new, deep Chandra data with radio and
optical imaging. We will image each jet with sufficient sensitivity to
estimate beaming factors and magnetic fields in several distinct
regions, and so map the variations in these parameters down the jets.
HST observations will help diagnose the role of synchrotron emission
in the overall SED, and may reveal condensations on scales less than
0.1 arcsec.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;COS/NUV/FUV 11728&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;The Impact of Starbursts on the Gaseous Halos of Galaxies
&lt;/p&gt;&lt;p&gt;Perhaps the most important (yet uncertain) aspects of galaxy evolution
are the processes by which galaxies accrete gas and by which the
resulting star formation and black hole growth affects this accreting
gas. It is believed that both the form of the accretion and the nature
of the feedback change as a function of the galaxy mass. At low mass
the gas comes in cold and the feedback is provided by massive stars.
At high mass, the gas comes in hot, and the feedback is from an AGN.
The changeover occurs near the mass where the galaxy population
transitions from star-forming galaxies to red and dead ones. The
population of red and dead galaxies is building with cosmic time, and
it is believed that feedback plays an important role in this process:
shutting down star formation by heating and/or expelling the reservoir
of cold halo gas. To investigate these ideas, we propose to use COS
far-UV spectra of background QSOs to measure the properties of the
halo gas in a sample of galaxies near the transition mass that have
undergone starbursts within the past 100 Myr to 1 Gyr. The galactic
wind associated with the starburst is predicted to have affected the
properties of the gaseous halo. To test this, we will compare the
properties of the halos of the post-starburst galaxies to those of a
control sample of galaxies matched in mass and QSO impact parameter.
Do the halos of the post-starburst galaxies show a higher incidence
rate of Ly-Alpha and metal absorption-lines? Are the kinematics of the
halo gas more disturbed in the post-starbursts? Has the wind affected
the ionization state and/or the metallicity of the halo? These data
will provide fresh new insights into the role of feedback from massive
stars on the evolution of galaxies, and may also offer clues about the
properties of the QSO metal absorption-line systems at high-redshift .
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/IR 11712&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Calibration of Surface Brightness Fluctuations for WFC3/IR
&lt;/p&gt;&lt;p&gt;We aim to characterize galaxy surface brightness fluctuations (SBF),
and calibrate the SBF distance method, in the F110W and F160W filters
of the Wide Field Camera 3 IR channel. Because of the very high
throughput of F110W and the good match of F160W to the standard H
band, we anticipate that both of these filters will be popular choices
for galaxy observations with WFC3/IR. The SBF signal is typically an
order of magnitude brighter in the near-IR than in the optical, and
the characteristics (sensitivity, FOV, cosmetics) of the WFC3/IR
channel will be enormously more efficient for SBF measurements than
previously available near-IR cameras. As a result, our proposed SBF
calibration will allow accurate distance derivation whenever an
early-type or bulge-dominated galaxy is observed out to a distance of
150 Mpc or more (i.e., out to the Hubble flow) in the calibrated
passbands. For individual galaxy observations, an accurate distance is
useful for establishing absolute luminosities, black hole masses,
linear sizes, etc. Eventually, once a large number of galaxies have
been observed across the sky with WFC3/IR, this SBF calibration will
enable accurate mapping of the total mass density distribution in the
local universe using the data available in the HST archive. The
proposed observations will have additional important scientific value;
in particular, we highlight their usefulness for understanding the
nature of multimodal globular cluster color distributions in giant
elliptical galaxies.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UVIS 11697&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Proper Motion Survey of Classical and SDSS Local Group Dwarf Galaxies
&lt;/p&gt;&lt;p&gt;Using the superior resolution of HST, we propose to continue our
proper motion survey of Galactic dwarf galaxies. The target galaxies
include one classical dwarf, Leo II, and six that were recently
identified in the Sloan Digital Sky Survey data: Bootes I, Canes
Venatici I, Canes Venatici II, Coma Berenices, Leo IV, and Ursa Major
II. We will observe a total of 16 fields, each centered on a
spectroscopically-confirmed QSO. Using QSOs as standards of rest in
measuring absolute proper motions has proven to be the most accurate
and most efficient method. HST is our only option to quickly determine
the space motions of the SDSS dwarfs because suitable ground-based
imaging is only a few years old and such data need several decades to
produce a proper motion. The two most distant galaxies in our sample
will require time baselines of four years to achieve our goal of a
30-50 km/s uncertainty in the tangential velocity; given this and the
finite lifetime of HST, it is imperative that first-epoch observations
be taken in this cycle. The SDSS dwarfs have dramatically lower
surface brightnesses and luminosities than the classical dwarfs.
Proper motions are crucial for determining orbits of the galaxies and
knowing the orbits will allow us to test theories for the formation
and evolution of these galaxies and, more generally, for the formation
of the Local Group.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/IR 11696&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Infrared Survey of Star Formation Across Cosmic Time
&lt;/p&gt;&lt;p&gt;We propose to use the unique power of WFC3 slitless spectroscopy to
measure the evolution of cosmic star formation from the end of the
reionization epoch at z&amp;#62;6 to the close of the galaxy- building era at
z~0.3.Pure parallel observations with the grisms have proven to be
efficient for identifying line emission from galaxies across a broad
range of redshifts. The G102 grism on WFC3 was designed to extend this
capability to search for Ly-alpha emission from the first galaxies.
Using up to 250 orbits of pure parallel WFC3 spectroscopy, we will
observe about 40 deep (4-5 orbit) fields with the combination of G102
and G141, and about 20 shallow (2-3 orbit) fields with G141 alone.
&lt;/p&gt;&lt;p&gt;Our primary science goals at the highest redshifts are: (1) Detect Lya
in ~100 galaxies with z&amp;#62;5.6 and measure the evolution of the Lya
luminosity function, independent of of cosmic variance; 2) Determine
the connection between emission line selected and continuum-break
selected galaxies at these high redshifts, and 3) Search for the
proposed signature of neutral hydrogen absorption at re-ionization. At
intermediate redshifts we will (4) Detect more than 1000 galaxies in
Halpha at 0.5&amp;#60;z&amp;#60;1.8 to measure the evolution of the
extinction-corrected star formation density across the peak epoch of
star formation. This is over an order-of-magnitude improvement in the
current statistics, from the NICMOS Parallel grism survey. (5) Trace
``cosmic downsizing&amp;#34; from 0.5&amp;#60;z&amp;#60;2.2; and (6) Estimate the evolution in
reddening and metallicty in star- forming galaxies and measure the
evolution of the Seyfert population. For hundreds of spectra we will
be able to measure one or even two line pair ratios -- in particular,
the Balmer decrement and / are sensitive to gas reddening
and metallicity. As a bonus, the G102 grism offers the possibility of
detecting Lya emission at z=7-8.8.
&lt;/p&gt;&lt;p&gt;To identify single-line Lya emitters, we will exploit the wide
0.8--1.9um wavelength coverage of the combined G102+G141 spectra. All
 and  interlopers detected in G102 will be reliably
separated from true LAEs by the detection of at least one strong line
in the G141 spectrum, without the need for any ancillary data. We
waive all proprietary rights to our data and will make high-level data
products available through the ST/ECF.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;COS/FUV 11687&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;SNAPing Coronal Iron
&lt;/p&gt;&lt;p&gt;This is a Snapshot Survey to explore two forbidden lines of highly
ionized iron in late-type coronal sources. Fe XII 1349 (T~ 2 MK) and
Fe XXI 1354 (T~ 10 MK) -- well known to Solar Physics -- have been
detected in about a dozen cool stars, mainly with HST/STIS. The UV
coronal forbidden lines are important because they can be observed
with velocity resolution of better than 15 km/s, whereas even the
state-of-the-art X-ray spectrometers on Chandra can manage only 300
km/s in the kilovolt band where lines of highly ionized iron more
commonly are found. The kinematic properties of hot coronal plasmas,
which are of great interest to theorists and modelers, thus only are
accessible in the UV at present. The bad news is that the UV coronal
forbidden lines are faint, and were captured only in very deep
observations with STIS. The good news is that 3rd-generation Cosmic
Origins Spectrograph, slated for installation in HST by SM4, in a mere
25 minute exposure with its G130M mode can duplicate the sensitivity
of a landmark 25-orbit STIS E140M observation of AD Leo, easily the
deepest such exposure of a late-type star so far. Our goal is to build
up understanding of the properties of Fe XII and Fe XXI in additional
objects beyond the current limited sample: how the lineshapes depend
on activity, whether large scale velocity shifts can be detected, and
whether the dynamical content of the lines can be inverted to map the
spatial morphology of the stellar corona (as in &amp;#34;Doppler Imaging'').
In other words, we want to bring to bear in the coronal venue all the
powerful tricks of spectroscopic remote sensing, well in advance of
the time that this will be possible exploiting the corona's native
X-ray radiation. The 1290-1430 band captured by side A of G130M also
contains a wide range of key plasma diagnostics that form at
temperatures from below 10, 000 K (neutral lines of CNO), to above
200, 000 K (semi-permitted O V 1371), including the important bright
multiplets of C II at 1335 and Si IV at 1400; yielding a diagnostic
gold mine for the subcoronal atmosphere. Because of the broad value of
the SNAP spectra, beyond the coronal iron project, we waive the normal
proprietary rights.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/IR 11666&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Chilly Pairs: A Search for the Latest-type Brown Dwarf Binaries and
the Prototype Y Dwarf
&lt;/p&gt;&lt;p&gt;We propose to use HST/WFC3 to image a sample of 27 of the nearest (&amp;#60;
20 pc) and lowest luminosity T-type brown dwarfs in order to identify
and characterize new very low mass binary systems. Only 3 late-type T
dwarf binaries have been found to date, despite that fact that these
systems are critical benchmarks for evolutionary and atmospheric
models at the lowest masses. They are also the most likely systems to
harbor Y dwarf companions, an as yet unpopulated putative class of
very cold (T &amp;#60; 600 K) brown dwarfs. Our proposed program will more
than double the number of T5-T9 dwarfs imaged at high resolution, with
an anticipated yield of ~5 new binaries with initial characterization
of component spectral types. We will be able to probe separations
sufficient to identify systems suitable for astrometric orbit and
dynamical mass measurements. We also expect one of our discoveries to
contain the first Y-type brown dwarf. Our proposed program complements
and augments ongoing ground-based adaptive optics surveys and provides
pathway science for JWST.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UVIS 11661&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;The Black Hole Mass - Bulge Luminosity Relationship for the Nearest
Reverberation-Mapped AGNs
&lt;/p&gt;&lt;p&gt;We propose to obtain WFC3 host galaxy images of the eight nearest AGNs
with masses from reverberation mapping, and one star as a PSF model.
These images will allow us to determine with unprecedented accuracy
the bulge luminosities of the host galaxies, a goal which is not
achievable from the ground due to the blurring of the very bright PSF
component under typical, and even very good, seeing conditions.
High-resolution ACS images of the host galaxies of more luminous AGNs
reveal that the black hole mass-bulge luminosity and black hole
mass-bulge mass relationships for AGNs are not well constrained and
arise from what appear to be fundamentally flawed data sets. With the
addition of the images proposed here to our current sample of ACS
images, we will be able to extend our determinations of the black hole
mass- bulge luminosity and black hole mass-bulge mass relationships
for AGNs by an order of magnitude and test our preliminary results for
these fundamentally important relationships against those previously
determined for quiescent galaxies.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;COS/NUV/ACS/WFC/FUV 11658&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Probing the Outer Regions of M31 with QSO Absorption Lines
&lt;/p&gt;&lt;p&gt;We propose HST-COS spectroscopy of 10 quasars behind M31. Absorption
lines due to MgII, FeII, CIV, and a variety of other lines will be
searched for and measured. Six quasars lie between 1 and 4.2 Holmberg
radii near the major axis on the southwest side, where confusion with
Milky Way gas is minimized. Two lie even farther out on the southwest
side of the major axis. One lies within 1 Holmberg radius. Two of the
10 pass through M31's high velocity clouds seen in a detailed 21 cm
emission map. Exposure time estimates were based on SDSS magnitudes
and available GALEX magnitudes. Thus, using the most well-studied
external spiral galaxy in the sky, our observations will permit us to
check, better than ever before, the standard picture that quasar
metal-line absorption systems such as MgII and CIV arise in an
extended gaseous halo/disk of a galaxy well beyond its observable
optical radius. The observations will yield insights into the nature
of the gas and its connection to the very extended stellar components
of M31 that have recently been studied. Notably the observations have
the potential of extending M31's rotation curve to very large
galactocentric distances, thereby placing new constraints on M31's
dark matter halo.
&lt;/p&gt;&lt;p&gt;Finally, we also request that the coordinated parallel orbits be
allocated to this program so that we may image the resolved stellar
content of M31's halo and outer disk.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/IR 11631&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Binary Brown Dwarfs and the L/T Transition
&lt;/p&gt;&lt;p&gt;Brown dwarfs traverse spectral types M, L and T as their atmospheric
structure evolves and they cool into oblivion. This SNAPSHOT program
will obtain WFC3-IR images of 45 nearby late-L and early-T dwarfs to
investigate the nature of the L/T transition. Recent analyses have
suggested that a substantial proportion of late-L and early-T dwarfs
are binaries, comprised of an L dwarf primary and T dwarf secondary.
WFC3-IR observations will let us quantify this suggestion by expanding
coverage to a much larger sample, and permitting comparison of the L/T
binary fraction against 'normal' ultracool dwarfs. Only eight L/T
binaries are currently known, including several that are poorly
resolved: we anticipate at least doubling the number of resolved
systems. The photometric characteristics of additional resolved
systems will be crucial to constraining theoretical models of these
late-type ultracool dwarfs. Finally, our data will also be eminently
suited to searching for extremely low luminosity companions,
potentially even reaching the Y dwarf regime.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/ACS/UVIS 11613&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;GHOSTS: Stellar Outskirts of Massive Spiral Galaxies
&lt;/p&gt;&lt;p&gt;We propose to continue our highly successful GHOSTS HST survey of the
resolved stellar populations of nearby, massive disk galaxies using
SNAPs. These observations provide star counts and color-magnitude
diagrams 2-3 magnitudes below the tip of the Red Giant Branch of the
outer disk and halo of each galaxy. We will measure the metallicity
distribution functions and stellar density profiles from star counts
down to very low average surface brightnesses, equivalent to ~32 V-mag
per square arcsec.
&lt;/p&gt;&lt;p&gt;This proposal will substantially improve our unique sampling of galaxy
outskirts. Our targets cover a range in galaxy mass, luminosity,
inclination, and morphology. As a function of these galaxy properties,
this survey provides: - the most extensive, systematic measurement of
radial light profiles and axial ratios of the diffuse stellar halos
and outer disks of spiral galaxies; - a comprehensive analysis of halo
metallicity distributions as function of galaxy type and position
within the galaxy; - an unprecedented study of the stellar metallicity
and age distribution in the outer disk regions where the disk
truncations occur; - the first comparative study of globular clusters
and their field stellar populations.
&lt;/p&gt;&lt;p&gt;We will use these fossil records of the galaxy assembly process to
test halo formation models within the hierarchical galaxy formation
scheme.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;COS/NUV/FUV 11598&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;How Galaxies Acquire their Gas: A Map of Multiphase Accretion and
Feedback in Gaseous Galaxy Halos
&lt;/p&gt;&lt;p&gt;We propose to address two of the biggest open questions in galaxy
formation - how galaxies acquire their gas and how they return it to
the IGM - with a concentrated COS survey of diffuse multiphase gas in
the halos of SDSS galaxies at z = 0.15 - 0.35. Our chief science goal
is to establish a basic set of observational facts about the physical
state, metallicity, and kinematics of halo gas, including the sky
covering fraction of hot and cold material, the metallicity of infall
and outflow, and correlations with galaxy stellar mass, type, and
color - all as a function of impact parameter from 10 - 150 kpc.
Theory suggests that the bimodality of galaxy colors, the shape of the
luminosity function, and the mass-metallicity relation are all
influenced at a fundamental level by accretion and feedback, yet these
gas processes are poorly understood and cannot be predicted robustly
from first principles. We lack even a basic observational assessment
of the multiphase gaseous content of galaxy halos on 100 kpc scales,
and we do not know how these processes vary with galaxy properties.
This ignorance is presently one of the key impediments to
understanding galaxy formation in general. We propose to use the
high-resolution gratings G130M and G160M on the Cosmic Origins
Spectrograph to obtain sensitive column density measurements of a
comprehensive suite of multiphase ions in the spectra of 43 z &amp;#60; 1 QSOs
lying behind 43 galaxies selected from the Sloan Digital Sky Survey.
In aggregate, these sightlines will constitute a statistically sound
map of the physical state and metallicity of gaseous halos, and
subsets of the data with cuts on galaxy mass, color, and SFR will seek
out predicted variations of gas properties with galaxy properties. Our
interpretation of these data will be aided by state-of-the-art
hydrodynamic simulations of accretion and feedback, in turn providing
information to refine and test such models. We will also use Keck,
MMT, and Magellan (as needed) to obtain optical spectra of the QSOs to
measure cold gas with Mg II, and optical spectra of the galaxies to
measure SFRs and to look for outflows. In addition to our other
science goals, these observations will help place the Milky Way's
population of multiphase, accreting High Velocity Clouds (HVCs) into a
global context by identifying analogous structures around other
galaxies. Our program is designed to make optimal use of the unique
capabilities of COS to address our science goals and also generate a
rich dataset of other absorption-line systems.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UVIS 11594&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;A WFC3 Grism Survey for Lyman Limit Absorption at z=2
&lt;/p&gt;&lt;p&gt;We propose to conduct a spectroscopic survey of Lyman limit absorbers
at redshifts 1.8 &amp;#60; z &amp;#60; 2.5, using WFC3 and the G280 grism. This
proposal intends to complete an approved Cycle 15 SNAP program
(10878), which was cut short due to the ACS failure. We have selected
64 quasars at 2.3 &amp;#60; z &amp;#60; 2.6 from the Sloan Digital Sky Survey
Spectroscopic Quasar Sample, for which no BAL signature is found at
the QSO redshift and no strong metal absorption lines are present at z
&lt;span class=&quot;quoted_reply&quot;&gt;&amp;#62; 2.3 along the lines of sight. The survey has three main&lt;/span&gt;
observational goals. First, we will determine the redshift frequency
dn/dz of the LLS over the column density range 16.0 &amp;#60; log(NHI) &amp;#60; 20.3
cm^-2. Second, we will measure the column density frequency
distribution f(N) for the partial Lyman limit systems (PLLS) over the
column density range 16.0 &amp;#60; log(NHI) &amp;#60; 17.5 cm^-2. Third, we will
identify those sightlines which could provide a measurement of the
primordial D/H ratio. By carrying out this survey, we can also help
place meaningful constraints on two key quantities of cosmological
relevance. First, we will estimate the amount of metals in the LLS
using the f(N), and ground based observations of metal line
transitions. Second, by determining f(N) of the PLLS, we can constrain
the amplitude of the ionizing UV background at z~2 to a greater
precision. This survey is ideal for a snapshot observing program,
because the on-object integration times are all well below 30 minutes,
and follow-up observations from the ground require minimal telescope
time due to the QSO sample being bright.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UVIS 11577&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Opening New Windows on the Antennae with WFC3
&lt;/p&gt;&lt;p&gt;We propose to use WFC3 to provide key observations of young star
clusters in &amp;#34;The Antennae&amp;#34; (NGC4038/39). Of prime importance is the
WFC3's ability to push the limiting UV magnitude FIVE mag deeper than
our previous WFPC2 observations. This corresponds to pushing the
limiting cluster mass from ~10**5 to ~10**3 solar masses for cluster
ages ~10**8 yrs. In addition, the much wider field of view of the WFC3
IR channel will allow us to map out both colliding disks rather than
just the Overlap Region between them. This will be especially
important for finding the youngest clusters that are still embedded in
their placental cocoons. The extensive set of narrow-band filters will
provide an effective means for determining the properties of shocks,
which are believed to be a primary triggering mechanism for star
formation. We will also use ACS in parallel with WFC3 to observe
portions of both the northern and southern tails at no additional
orbital cost. Finally, one additional primary WFC3 orbit will be used
to supplement exisiting HST observations of the star-forming &amp;#34;dwarf&amp;#34;
galaxy at the end of the southern tail. Hence, when completed we will
have full UBVI + H_alpha coverage (or more for the main galaxy) of
four different environments in the Antennae. In conjunction with the
extensive multi- wavelength database we have collected (both HST and
ground based) these observations will provide answers to fundamental
questions such as: How do these clusters form and evolve? How is star
formation triggered? How do star clusters affect the local and global
ISM, and the evolution of the galaxy as a whole? The Antennae galaxies
are the nearest example of a major disk--disk merger, and hence may
represent our best chance for understanding how mergers form
tremendous numbers of clusters and stars, both in the local universe
and during galaxy assembly at high redshift.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/CC/MA 11576&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Physical Parameters of the Upper Atmosphere of the Extrasolar Planet
HD209458b
&lt;/p&gt;&lt;p&gt;One of the most studied extrasolar planet, HD209458b, has revealed
both its lower and upper atmosphere thanks to HST and Spitzer
observatories.
&lt;/p&gt;&lt;p&gt;Through transmission spectroscopy technique, several atmospheric
species were detected: NaI, HI, OI and CII. Using STIS archived
transit absorption spectrum from 3000 to 8000 Angstrom, we obtained
detailed constraints on the vertical profile of temperature, pressure
and abundances (Sing et al 2008a, 2008b, Lecavelier et al. 2008b).
&lt;/p&gt;&lt;p&gt;By observing in the NUV, from 2300 to 3100 Angstrom, we expect to
obtain new constraints on the physical conditions and the chemical
composition of the upper atmosphere: temperature/pressure profile up
to very high in the atmosphere, abundance and condensation altitudes
of new species, and new insight in the atmospheric escape and
ionization state at the upper levels. The observation of four
HD209458b transits with a single E230M setting will give access to
many NUV atomic lines addressing these issues. The proposed
observations will probe, for the first time, in details the atmosphere
of a hot Jupiter, thus bench marking follow up studies.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/CCD 11567&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Boron Abundances in Rapidly Rotating Early-B Stars
&lt;/p&gt;&lt;p&gt;Models of rotation in early-B stars predict that rotationally driven
mixing should deplete surface boron abundances during the
main-sequence lifetime of many stars. However, recent work has shown
that many boron depleted stars are intrinsically slow rotators for
which models predict no depletion should have occurred, while
observations of nitrogen in some more rapidly rotating stars show less
mixing than the models predict. Boron can provide unique information
on the earliest stages of mixing in B stars, but previous surveys have
been biased towards narrow- lined stars because of the difficulty in
measuring boron abundances in rapidly rotating stars. The two targets
observed as part of our Cycle 13 SNAP program 10175, just before STIS
failed, demonstrate that it is possible to make useful boron abundance
measurements for early-B stars with Vsin(i) above 100 km/s. We propose
to extend that survey to a large enough sample of stars to allow
statistically significant tests of models of rotational mixing in
early-B stars.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/ACS/UVIS 11360&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Star Formation in Nearby Galaxies
&lt;/p&gt;&lt;p&gt;Star formation is a fundamental astrophysical process; it controls
phenomena ranging from the evolution of galaxies and nucleosynthesis
to the origins of planetary systems and abodes for life. The WFC3,
optimized at both UV and IR wavelengths and equipped with an extensive
array of narrow-band filters, brings unique capabilities to this area
of study. The WFC3 Scientific Oversight Committee (SOC) proposes an
integrated program on star formation in the nearby universe which will
fully exploit these new abilities. Our targets range from the
well-resolved R136 in 30 Dor in the LMC (the nearest super star
cluster) and M82 (the nearest starbursting galaxy) to about half a
dozen other nearby galaxies that sample a wide range of star-formation
rates and environments. Our program consists of broad band
multiwavelength imaging over the entire range from the UV to the
near-IR, aimed at studying the ages and metallicities of stellar
populations, revealing young stars that are still hidden by dust at
optical wavelengths, and showing the integrated properties of star
clusters. Narrow-band imaging of the same environments will allow us
to measure star-formation rates, gas pressure, chemical abundances,
extinction, and shock morphologies. The primary scientific issues to
be addressed are: (1) What triggers star formation? (2) How do the
properties of star-forming regions vary among different types of
galaxies and environments of different gas densities and compositions?
(3) How do these different environments affect the history of star
formation? (4) Is the stellar initial mass function universal or
determined by local conditions?
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/ACS/IR 11142&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Revealing the Physical Nature of Infrared Luminous Galaxies at
0.3&amp;#60;z&amp;#60;2.7 Using HST and Spitzer
&lt;/p&gt;&lt;p&gt;We aim to determine physical properties of IR luminous galaxies at
0.3&amp;#60;z&amp;#60;2.7 by requesting coordinated HST/NIC2 and MIPS 70um
observations of a unique, 24um flux-limited sample with complete
Spitzer mid-IR spectroscopy. The 150 sources investigated in this
program have S(24um) &amp;#62; 0.8mJy and their mid-IR spectra have already
provided the majority targets with spectroscopic redshifts
(0.3&amp;#60;z&amp;#60;2.7). The proposed 150~orbits of NIC2 and 66~hours of MIPS 70um
will provide the physical measurements of the light distribution at
the rest-frame ~8000A and better estimates of the bolometric
luminosity. Combining these parameters together with the rich suite of
spectral diagnostics from the mid-IR spectra, we will (1) measure how
common mergers are among LIRGs and ULIRGs at 0.3&amp;#60;z&amp;#60;2.7, and establish
if major mergers are the drivers of z&amp;#62;1 ULIRGs, as in the local
Universe, (2) study the co-evolution of star formation and blackhole
accretion by investigating the relations between the fraction of
starburst/AGN measured from mid-IR spectra vs. HST morphologies,
L(bol) and z, and (3) obtain the current best estimates of the far-IR
emission, thus L(bol) for this sample, and establish if the relative
contribution of mid-to-far IR dust emission is correlated with
morphology (resolved vs. unresolved).
&lt;/p&gt;


&lt;hr/&gt;
TOPIC: Daily Report #5141&lt;br/&gt;
&lt;a href=&quot;http://groups.google.com/group/sci.astro.hubble/t/081d819455fa1aa6?hl=en&quot;&gt;http://groups.google.com/group/sci.astro.hubble/t/081d819455fa1aa6?hl=en&lt;/a&gt;
&lt;hr/&gt;
&lt;p&gt;== 1 of 1 ==&lt;br/&gt;
Date: Tues, Jul 20 2010 8:46&amp;#194;&amp;#160;am 
From: &amp;#34;Bassford, Lynn&amp;#34;  
&lt;/p&gt;
&lt;p&gt;HUBBLE SPACE TELESCOPE - Continuing to Collect World Class Science
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;DAILY REPORT #5141&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;PERIOD COVERED: 5am July 19 - 5am July 20, 2010 (DOY 200/09:00z-201/09:00z)
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;FLIGHT OPERATIONS SUMMARY:&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Significant Spacecraft Anomalies: (The following are preliminary
reports of potential non-nominal performance that will be
investigated.)
&lt;/p&gt;&lt;dl&gt;
  &lt;dt&gt;HSTARS&lt;/dt&gt;
&lt;dd&gt;&lt;/dd&gt;&lt;/dl&gt;
&lt;p&gt;#12333 OBAD at 200/17:21:57z failed and GSAcq(1,2,1) at 200/17:26:57z
failed with search radius limit exceeded on FGS2
&lt;/p&gt;&lt;p&gt;Observations affected: Astrometry Proposal #12316
&lt;/p&gt;&lt;p&gt;From DOY 187:
&lt;/p&gt;&lt;p&gt;#12334 ReAcq(1,0,1) at 187/04:37:32z required two attempts for FL-DV
with scan step limit exceeded on FGS1
&lt;/p&gt;&lt;p&gt;COMPLETED OPS REQUEST: (None)
&lt;/p&gt;&lt;p&gt;COMPLETED OPS NOTES: (None)
&lt;/p&gt;&lt;pre&gt;
                             SCHEDULED      SUCCESSFUL
FGS GSAcq                     9               8
FGS REAcq                     7               7
OBAD with Maneuver            6               5&lt;/pre&gt;
&lt;p&gt;SIGNIFICANT EVENTS: (None)
&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;OBSERVATIONS SCHEDULED:&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;ACS/WFC 11996&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;CCD Daily Monitor (Part 3)
&lt;/p&gt;&lt;p&gt;This program comprises basic tests for measuring the read noise and
dark current of the ACS WFC and for tracking the growth of hot pixels.
The recorded frames are used to create bias and dark reference images
for science data reduction and calibration. This program will be
executed four days per week (Mon, Wed, Fri, Sun) for the duration of
Cycle 17. To facilitate scheduling, this program is split into three
proposals. This proposal covers 308 orbits (19.25 weeks) from 21 June
2010 to 1 November 2010.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;COS/FUV 11895&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;FUV Detector Dark Monitor
&lt;/p&gt;&lt;p&gt;Monitor the FUV detector dark rate by taking long science exposures
without illuminating the detector. The detector dark rate and spatial
distribution of counts will be compared to pre-launch and SMOV data in
order to verify the nominal operation of the detector. Variations of
count rate as a function of orbital position will be analyzed to find
dependence of dark rate on proximity to the SAA. Dependence of dark
rate as function of time will also be tracked.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;COS/NUV/FUV 11598&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;How Galaxies Acquire their Gas: A Map of Multiphase Accretion and
Feedback in Gaseous Galaxy Halos
&lt;/p&gt;&lt;p&gt;We propose to address two of the biggest open questions in galaxy
formation - how galaxies acquire their gas and how they return it to
the IGM - with a concentrated COS survey of diffuse multiphase gas in
the halos of SDSS galaxies at z = 0.15 - 0.35. Our chief science goal
is to establish a basic set of observational facts about the physical
state, metallicity, and kinematics of halo gas, including the sky
covering fraction of hot and cold material, the metallicity of infall
and outflow, and correlations with galaxy stellar mass, type, and
color - all as a function of impact parameter from 10 - 150 kpc.
Theory suggests that the bimodality of galaxy colors, the shape of the
luminosity function, and the mass-metallicity relation are all
influenced at a fundamental level by accretion and feedback, yet these
gas processes are poorly understood and cannot be predicted robustly
from first principles. We lack even a basic observational assessment
of the multiphase gaseous content of galaxy halos on 100 kpc scales,
and we do not know how these processes vary with galaxy properties.
This ignorance is presently one of the key impediments to
understanding galaxy formation in general. We propose to use the
high-resolution gratings G130M and G160M on the Cosmic Origins
Spectrograph to obtain sensitive column density measurements of a
comprehensive suite of multiphase ions in the spectra of 43 z &amp;#60; 1 QSOs
lying behind 43 galaxies selected from the Sloan Digital Sky Survey.
In aggregate, these sightlines will constitute a statistically sound
map of the physical state and metallicity of gaseous halos, and
subsets of the data with cuts on galaxy mass, color, and SFR will seek
out predicted variations of gas properties with galaxy properties. Our
interpretation of these data will be aided by state-of-the-art
hydrodynamic simulations of accretion and feedback, in turn providing
information to refine and test such models. We will also use Keck,
MMT, and Magellan (as needed) to obtain optical spectra of the QSOs to
measure cold gas with Mg II, and optical spectra of the galaxies to
measure SFRs and to look for outflows. In addition to our other
science goals, these observations will help place the Milky Way's
population of multiphase, accreting High Velocity Clouds (HVCs) into a
global context by identifying analogous structures around other
galaxies. Our program is designed to make optimal use of the unique
capabilities of COS to address our science goals and also generate a
rich dataset of other absorption-line systems.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;FGS 12316&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;HST/FGS Astrometric Search for Young Planets Around Beta Pic and AU
Mic
&lt;/p&gt;&lt;p&gt;AU Mic is a nearby Vega-type debris disk stars. Its disk system has
been spatially resolved in exquisite detail, predominantly via the ACS
coronagraph and WFPC-2 cameras onboard HST. These images exhibit a
wealth of morphological features which provide compelling indirect
evidence that AU Mic likely harbors short-period planetary body(ies).
We propose to use the superlative astrometric capabilities of HST/FGS
to directly detect these planets, hence provide the first direct
planet detection in a Vega-type system whose disk has been imaged at
high spatial resolution.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/CC 11845&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;CCD Dark Monitor Part 2
&lt;/p&gt;&lt;p&gt;Monitor the darks for the STIS CCD.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/CC 11847&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;CCD Bias Monitor-Part 2
&lt;/p&gt;&lt;p&gt;Monitor the bias in the 1x1, 1x2, 2x1, and 2x2 bin settings at gain=1,
and 1x1 at gain = 4, to build up high-S/N superbiases and track the
evolution of hot columns.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/CCD 11721&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Verifying the Utility of Type Ia Supernovae as Cosmological Probes:
Evolution and Dispersion in the Ultraviolet Spectra
&lt;/p&gt;&lt;p&gt;The study of distant type Ia supernova (SNe Ia) offers the most
practical and immediate discriminator between popular models of dark
energy. Yet fundamental questions remain over possible
redshift-dependent trends in their observed and intrinsic properties.
High-quality Keck spectroscopy of a representative sample of 36
intermediate redshift SNe Ia has revealed a surprising, and
unexplained, diversity in their rest-frame UV fluxes. One possible
explanation is hitherto undiscovered variations in the progenitor
metallicity. Unfortunately, this result cannot be compared to local UV
data as only two representative SNe Ia have been studied near maximum
light. Taking advantage of two new `rolling searches' and the
restoration of STIS, we propose a non-disruptive TOO campaign to
create an equivalent comparison local sample. This will allow us to
address possible evolution in the mean UV spectrum and its diversity,
an essential precursor to the study of SNe beyond z~1.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/CCD/MA2 11568&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;A SNAPSHOT Survey of the Local Interstellar Medium: New NUV
Observations of Stars with Archived FUV Observations
&lt;/p&gt;&lt;p&gt;We propose to obtain high-resolution STIS E230H SNAP observations of
MgII and FeII interstellar absorption lines toward stars within 100
parsecs that already have moderate or high-resolution far-UV (FUV),
900-1700 A, observations available in the MAST Archive. Fundamental
properties, such as temperature, turbulence, ionization, abundances,
and depletions of gas in the local interstellar medium (LISM) can be
measured by coupling such observations. Due to the wide spectral range
of STIS, observations to study nearby stars also contain important
data about the LISM embedded within their spectra. However, unlocking
this information from the intrinsically broad and often saturated FUV
absorption lines of low-mass ions, (DI, CII, NI, OI), requires first
understanding the kinematic structure of the gas along the line of
sight. This can be achieved with high resolution spectra of high-mass
ions, (FeII, MgII), which have narrow absorption lines, and can
resolve each individual velocity component (interstellar cloud). By
obtaining short (~10 minute) E230H observations of FeII and MgII, for
stars that already have moderate or high- resolution FUV spectra, we
can increase the sample of LISM measurements, and thereby expand our
knowledge of the physical properties of the gas in our galactic
neighborhood. STIS is the only instrument capable of obtaining the
required high resolution data now or in the foreseeable future.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;STIS/MA1/MA2 11857&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;STIS Cycle 17 MAMA Dark Monitor
&lt;/p&gt;&lt;p&gt;This proposal monitors the behavior of the dark current in each of the
MAMA detectors.
&lt;/p&gt;&lt;p&gt;The basic monitor takes two 1380s ACCUM darks each week with each
detector. However, starting Oct 5, pairs are only included for weeks
that the LRP has external MAMA observations planned. The weekly pairs
of exposures for each detector are linked so that they are taken at
opposite ends of the same SAA free interval. This pairing of exposures
will make it easier to separate long and short term temporal
variability from temperature dependent changes.
&lt;/p&gt;&lt;p&gt;For both detectors, additional blocks of exposures are taken once
every six months. These are groups of five 1314s FUV-MAMA Time-Tag
darks or five 3x315s NUV ACCUM darks distributed over a single
SAA-free interval. This will give more information on the brightness
of the FUV MAMA dark current as a function of the amount of time that
the HV has been on, and for the NUV MAMA will give a better measure of
the short term temperature dependence.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/ACS/UVIS/IR 11570&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Narrowing in on the Hubble Constant and Dark Energy
&lt;/p&gt;&lt;p&gt;A measurement of the Hubble constant to a precision of a few percent
would be a powerful aid to the investigation of the nature of dark
energy and a potent &amp;#34;end-to end&amp;#34; test of the present cosmological
model. In Cycle 15 we constructed a new streamlined distance ladder
utilizing high- quality type Ia supernova data and observations of
Cepheids with HST in the near-IR to minimize the dominant sources of
systematic uncertainty in past measurements of the Hubble constant and
reduce its total uncertainty to a little under 5%. Here we propose to
exploit this new route to reduce the remaining uncertainty by more
than 30%, translating into an equal reduction in the uncertainty of
the equation of state of dark energy. We propose three sets of
observations to reach this goal: a mosaic of NGC 4258 with WFC3 in
F160W to triple its sample of long period Cepheids, WFC3/F160W
observations of the 6 ideal SN Ia hosts to triple their samples of
Cepheids, and observations of NGC 5584 the host of a new SN Ia, SN
2007af, to discover and measure its Cepheids and begin expanding the
small set of SN Ia luminosity calibrations. These observations would
provide the bulk of a coordinated program aimed at making the
measurement of the Hubble constant one of the leading constraints on
dark energy.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/IR 11591&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Are Low-Luminosity Galaxies Responsible for Cosmic Reionization?
&lt;/p&gt;&lt;p&gt;Our group has demonstrated that massive clusters, acting as powerful
cosmic lenses, can constrain the abundance and properties of
low-luminosity star-forming sources beyond z~6; such sources are
thought to be responsible for ending cosmic reionization. The large
magnification possible in the critical regions of well-constrained
clusters brings sources into view that lie at or beyond the limits of
conventional exposures such as the UDF. We have shown that the
combination of HST and Spitzer is particularly effective in delivering
the physical properties of these distant sources, constraining their
mass, age and past star formation history. Indirectly, we therefore
gain a valuable glimpse to yet earlier epochs. Recognizing the result
(and limitations) of blank field surveys, we propose a systematic
search through 10 lensing clusters with ACS/F814W and
WFC3/[F110W+F160W] (in conjunction with existing deep IRAC data). Our
goal is to measure with great accuracy the luminosity function at z~7
over a range of at least 3 magnitude, based on the identification of
about 50 lensed galaxies at 6.5&amp;#60;z&amp;#60;8. Our survey will mitigate cosmic
variance and extend the search both to lower luminosities and, by
virtue of the WFC3/IRAC combination, to higher redshift. Thanks to the
lensing amplification spectroscopic follow-up will be possible and
make our findings the most robust prior to the era of JWST and the
ELTs.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/IR 11666&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Chilly Pairs: A Search for the Latest-type Brown Dwarf Binaries and
the Prototype Y Dwarf
&lt;/p&gt;&lt;p&gt;We propose to use HST/WFC3 to image a sample of 27 of the nearest (&amp;#60;
20 pc) and lowest luminosity T-type brown dwarfs in order to identify
and characterize new very low mass binary systems. Only 3 late-type T
dwarf binaries have been found to date, despite that fact that these
systems are critical benchmarks for evolutionary and atmospheric
models at the lowest masses. They are also the most likely systems to
harbor Y dwarf companions, an as yet unpopulated putative class of
very cold (T &amp;#60; 600 K) brown dwarfs. Our proposed program will more
than double the number of T5-T9 dwarfs imaged at high resolution, with
an anticipated yield of ~5 new binaries with initial characterization
of component spectral types. We will be able to probe separations
sufficient to identify systems suitable for astrometric orbit and
dynamical mass measurements. We also expect one of our discoveries to
contain the first Y-type brown dwarf. Our proposed program complements
and augments ongoing ground-based adaptive optics surveys and provides
pathway science for JWST.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/IR/S/C 11929&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;IR Dark Current Monitor
&lt;/p&gt;&lt;p&gt;Analyses of ground test data showed that dark current signals are more
reliably removed from science data using darks taken with the same
exposure sequences as the science data, than with a single dark
current image scaled by desired exposure time. Therefore, dark current
images must be collected using all sample sequences that will be used
in science observations. These observations will be used to monitor
changes in the dark current of the WFC3-IR channel on a day-to-day
basis, and to build calibration dark current ramps for each of the
sample sequences to be used by Gos in Cycle 17. For each sample
sequence/array size combination, a median ramp will be created and
delivered to the calibration database system (CDBS).
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UV/ACS/WFC 11636&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;First Resolved Imaging of Escaping Lyman Continuum
&lt;/p&gt;&lt;p&gt;The emission from star-forming galaxies appears to be responsible for
reionization of the universe at z &amp;#62; 6. However, the models that
attempt to describe the detailed impact of high-redshift galaxies on
the surrounding inter-galactic medium (IGM) are strongly dependent
upon several uncertain parameters. Perhaps the most uncertain is the
fraction of HI-ionizing photons produced by young stars that escape
into the IGM. Most attempts to measure this &amp;#34;escape fraction&amp;#34; have
produced null results. Recently, a small subset of z~3 Lyman Break
Galaxies (LBGs) has been found exhibiting large escape fractions. It
remains unclear however, what differentiates them from other LBGs.
Several models attempt to explain how such a large fraction of
ionizing continuum can escape through the HI and dust in the ISM (eg.
&amp;#34;chimneys&amp;#34; created by SNe winds, globular cluster formation, etc.),
each producing unique signatures which can be observed with resolved
imaging of the escaping Lyman continuum. To date, there are only six
LBGs with individual detections of escaping Lyman continuum at any
redshift. We propose a single deep, high resolution WFC3/UVIS image of
the ionizing continuum (F336W) and the rest-frame UV/optical
(F606W/F814W/F160W) of five of these six LBGs with large escape
fractions. These LBGs have a high surface density and large escape
fractions, and lie at the optimal redshift for Lyman continuum imaging
with UVIS filters, making our sample especially suitable for
follow-up. With these data we will discern the mechanisms responsible
for producing large escape fractions, and therefore gain insight into
the process of reionization.
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UVIS 11905&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;WFC3 UVIS CCD Daily Monitor
&lt;/p&gt;&lt;p&gt;The behavior of the WFC3 UVIS CCD will be monitored daily with a set
of full-frame, four-amp bias and dark frames. A smaller set of 2Kx4K
subarray biases are acquired at less frequent intervals throughout the
cycle to support subarray science observations. The internals from
this proposal, along with those from the anneal procedure (Proposal
11909), will be used to generate the necessary superbias and superdark
reference files for the calibration pipeline (CDBS).
&lt;/p&gt;&lt;p&gt;&lt;strong&gt;WFC3/UVIS 11908&lt;/strong&gt;
&lt;/p&gt;&lt;p&gt;Cycle 17: UVIS Bowtie Monitor
&lt;/p&gt;&lt;p&gt;Ground testing revealed an intermittent hysteresis type effect in the
UVIS detector (both CCDs) at the level of ~1%, lasting hours to days.
Initially found via an unexpected bowtie-shaped feature in flatfield
ratios, subsequent lab tests on similar e2v devices have since shown
that it is also present as simply an overall offset across the entire
CCD, i.e., a QE offset without any discernable pattern. These lab
tests have further revealed that overexposing the detector to count
levels several times full well fills the traps and effectively
neutralizes the bowtie. Each visit in this proposal acquires a set of
three 3x3 binned internal flatfields: the first unsaturated image will
be used to detect any bowtie, the second, highly exposed image will
neutralize the bowtie if it is present, and the final image will allow
for verification that the bowtie is gone.
&lt;/p&gt;

&lt;hr/&gt;
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  <entry>
    <title>Daily Report #5141</title>
    <link rel="alternate" href="http://www.aus-city.com/cgi-bin/dada/mail.cgi/archive/HST_REPORTS/20100721100503/"/>
    <id>tag:www.aus-city.com,2010-07-21:%2Fcgi-bin%2Fdada%2Fmail.cgi%2Farchive%2FHST_REPORTS%2F20100721100503%2F</id>
    
    <published>2010-07-21T10:05:03Z</published>
    <updated>2010-07-21T10:05:03Z</updated>
    <content type="html">

&lt;div class=WordSection1&gt;

&lt;p class=MsoNormal&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;HUBBLE
SPACE TELESCOPE - Continuing to Collect World Class Science &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;DAILY
REPORT #5141 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;PERIOD
COVERED: 5am July 19 - 5am July 20, 2010 (DOY 200/09:00z-201/09:00z) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;FLIGHT
OPERATIONS SUMMARY: &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Significant
Spacecraft Anomalies: (The following are preliminary reports&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;of
potential non-nominal performance that will be investigated.) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;HSTARS:&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;#12333 OBAD
at 200/17:21:57z failed and GSAcq(1,2,1) at 200/17:26:57z&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&amp;#160;&amp;#160; &amp;#160;failed with search radius limit exceeded on FGS2 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&amp;#160; &amp;#160;&amp;#160;Observations affected: Astrometry Proposal #12316&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;From DOY
187:&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;#12334
ReAcq(1,0,1) at 187/04:37:32z required two attempts for FL-DV with scan&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&amp;#160; &amp;#160;&amp;#160;step limit exceeded on FGS1 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COMPLETED
OPS REQUEST: (None) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COMPLETED
OPS NOTES: (None) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&amp;#160;
&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;SCHEDULED&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
SUCCESSFUL&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160; &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;FGS
GSAcq&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
9&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
8&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;FGS
REAcq&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
7&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
7&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160; &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;OBAD with
Maneuver&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&amp;#160;6&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
5&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;
&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;SIGNIFICANT
EVENTS: (None) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;OBSERVATIONS
SCHEDULED: &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;ACS/WFC
11996 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;CCD Daily
Monitor (Part 3) &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;This
program comprises basic tests for measuring the read noise and dark&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;current of
the ACS WFC and for tracking the growth of hot pixels. The&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;recorded
frames are used to create bias and dark reference images for&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;science
data reduction and calibration. This program will be executed&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;four days
per week (Mon, Wed, Fri, Sun) for the duration of Cycle 17. To&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;facilitate
scheduling, this program is split into three proposals. This&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;proposal
covers 308 orbits (19.25 weeks) from 21 June 2010 to 1 November&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;2010. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COS/FUV
11895 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;FUV
Detector Dark Monitor &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Monitor the
FUV detector dark rate by taking long science exposures&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;without
illuminating the detector. The detector dark rate and spatial&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;distribution
of counts will be compared to pre-launch and SMOV data in&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;order to
verify the nominal operation of the detector. Variations of&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;count rate
as a function of orbital position will be analyzed to find&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;dependence
of dark rate on proximity to the SAA. Dependence of dark rate&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;as function
of time will also be tracked. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;COS/NUV/FUV
11598 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;How
Galaxies Acquire their Gas: A Map of Multiphase Accretion and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Feedback in
Gaseous Galaxy Halos &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;We propose
to address two of the biggest open questions in galaxy&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;formation -
how galaxies acquire their gas and how they return it to the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;IGM - with
a concentrated COS survey of diffuse multiphase gas in the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;halos of
SDSS galaxies at z = 0.15 - 0.35. Our chief science goal is to&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;establish a
basic set of observational facts about the physical state,&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;metallicity,
and kinematics of halo gas, including the sky covering&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;fraction of
hot and cold material, the metallicity of infall and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;outflow,
and correlations with galaxy stellar mass, type, and color -&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;all as a
function of impact parameter from 10 - 150 kpc. Theory suggests&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;that the
bimodality of galaxy colors, the shape of the luminosity&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;function,
and the mass-metallicity relation are all influenced at a&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;fundamental
level by accretion and feedback, yet these gas processes are&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;poorly
understood and cannot be predicted robustly from first&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;principles.
We lack even a basic observational assessment of the&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;multiphase
gaseous content of galaxy halos on 100 kpc scales, and we do&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;not know
how these processes vary with galaxy properties. This ignorance&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;is
presently one of the key impediments to understanding galaxy&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;formation
in general. We propose to use the high-resolution gratings&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;G130M and
G160M on the Cosmic Origins Spectrograph to obtain sensitive&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;column
density measurements of a comprehensive suite of multiphase ions&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;in the
spectra of 43 z &amp;#60; 1 QSOs lying behind 43 galaxies selected from&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;the Sloan
Digital Sky Survey. In aggregate, these sightlines will&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;constitute
a statistically sound map of the physical state and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;metallicity
of gaseous halos, and subsets of the data with cuts on&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;galaxy
mass, color, and SFR will seek out predicted variations of gas&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;properties
with galaxy properties. Our interpretation of these data will&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;be aided by
state-of-the-art hydrodynamic simulations of accretion and&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;feedback,
in turn providing information to refine and test such models.&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;We will
also use Keck, MMT, and Magellan (as needed) to obtain optical&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;spectra of
the QSOs to measure cold gas with Mg II, and optical spectra&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;of the
galaxies to measure SFRs and to look for outflows. In addition to&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;our other
science goals, these observations will help place the Milky&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Way's
population of multiphase, accreting High Velocity Clouds (HVCs)&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;into a
global context by identifying analogous structures around other&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;galaxies.
Our program is designed to make optimal use of the unique&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;capabilities
of COS to address our science goals and also generate a&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;rich
dataset of other absorption-line systems. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;FGS 12316 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;HST/FGS
Astrometric Search for Young Planets Around Beta Pic and AU Mic &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;AU Mic is a
nearby Vega-type debris disk stars. Its disk system has been&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;spatially resolved
in exquisite detail, predominantly via the ACS&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;coronagraph
and WFPC-2 cameras onboard HST. These images exhibit a&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;wealth of
morphological features which provide compelling indirect&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;evidence
that AU Mic likely harbors short-period planetary body(ies). We&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;propose to
use the superlative astrometric capabilities of HST/FGS to&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;directly
detect these planets, hence provide the first direct planet&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;detection
in a Vega-type system whose disk has been imaged at high&lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;spatial
resolution. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;STIS/CC
11845 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;CCD Dark
Monitor Part 2 &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;&lt;o:p&gt;&amp;#160;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quot;sans-serif&quot;'&gt;Monitor the
darks for the STIS CCD. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;

&lt;p class=MsoNormal&gt;&lt;span style='font-family:&quot;Verdana&quot;,&quo