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#49893
Tue 14 Sep 2010 01:12:PM
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Joined: Feb 2001
Posts: 381,903
Launch Director
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OP
Launch Director
Joined: Feb 2001
Posts: 381,903 |
HUBBLE SPACE TELESCOPE - Continuing to Collect World Class Science
DAILY REPORT #5180
PERIOD COVERED: 5am September 13 - 5am September 14, 2010 (DOY 256/09:00z-257/09:00z)
FLIGHT OPERATIONS SUMMARY:
Significant Spacecraft Anomalies: (The following are preliminary reports
of potential non-nominal performance that will be investigated.)
HSTARS:
12402 - COS 1021 STB Message received at 257/01:22z, following successful
GSAcq (2,1,1) at 257/01:15:46z, indicating take data flag was down when a target
acquisition macro was about to make a slew request.
Observations possibly affected: WFC3 20-21 Proposal ID#11905.
COMPLETED OPS REQUEST: (None)
COMPLETED OPS NOTES: (None)
SCHEDULED SUCCESSFUL
FGS GSAcq 7 7
FGS REAcq 9 9
OBAD with Maneuver 3 3
SIGNIFICANT EVENTS: None.
OBSERVATIONS SCHEDULED:
ACS/WFC 11996
CCD Daily Monitor (Part 3)
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.
ACS/WFC 12210
SLACS for the Masses: Extending Strong Lensing to Lower Masses and
Smaller Radii
Strong gravitational lensing provides the most accurate possible
measurement of mass in the central regions of early-type galaxies
(ETGs). We propose to continue the highly productive Sloan Lens ACS
(SLACS) Survey for strong gravitational lens galaxies by observing a
substantial fraction of 135 new ETG gravitational-lens candidates with
HST-ACS WFC F814W Snapshot imaging. The proposed target sample has been
selected from the seventh and final data release of the Sloan Digital
Sky Survey, and is designed to complement the distribution of previously
confirmed SLACS lenses in lens-galaxy mass and in the ratio of Einstein
radius to optical half-light radius. The observations we propose will
lead to a combined SLACS sample covering nearly two decades in mass,
with dense mapping of enclosed mass as a function of radius out to the
half-light radius and beyond. With this longer mass baseline, we will
extend our lensing and dynamical analysis of the mass structure and
scaling relations of ETGs to galaxies of significantly lower mass, and
directly test for a transition in structural and dark-matter content
trends at intermediate galaxy mass. The broader mass coverage will also
enable us to make a direct connection to the structure of well-studied
nearby ETGs as deduced from dynamical modeling of their line-of-sight
velocity distribution fields. Finally, the combined sample will allow a
more conclusive test of the current SLACS result that the intrinsic
scatter in ETG mass-density structure is not significantly correlated
with any other galaxy observables. The final SLACS sample at the
conclusion of this program will comprise approximately 130 lenses with
known foreground and background redshifts, and is likely to be the
largest confirmed sample of strong-lens galaxies for many years to come.
ACS/WFC 12292
SWELLS: Doubling the Number of Disk-dominated Edge-on Spiral Lens
Galaxies
The formation of realistic disk galaxies within the LCDM cosmology is
still largely an unsolved problem. Theory is now beginning to make
predictions for how dark matter halos respond to galaxy formation, and
for the properties of disk galaxies. Measuring the density profiles of
dark matter halos on galaxy scales is therefore a strong test for the
standard paradigm of galaxy formation, offering great potential for
discovery. However, the degeneracy between the stellar and dark matter
contributions to galaxy rotation curves remains a major obstacle. Strong
gravitational lensing, when combined with spatially resolved kinematics
and stellar population models, can solve this long-standing problem.
Unfortunately, this joint methodology could not be exploited until
recently due to the paucity of known edge-on spiral lenses. We have
developed and demonstrated an efficient technique to find exactly these
systems. During supplemental cycle-16 we discovered five new spiral lens
galaxies, suitable for rotation curve measurements. We propose
multi-color HST imaging of 16 candidates and 2 partially-imaged
confirmed systems, to measure a sample of eight new edge-on spiral
lenses. This program will at least double the number of known
disk-dominated systems. This is crucial for constraining the relative
contribution of the disk, bulge and dark halo to the total density
profile.
ACS/WFC3 11734
The Hosts of High Redshift Gamma-Ray Bursts
Gamma-ray bursts are the most luminous explosive events known, acting as
beacons to the high redshift universe. Long duration GRBs have their
origin in the collapse of massive stars and thus select star forming
galaxies across a wide range of redshift. Due to their bright afterglows
we can study the details of GRB host galaxies via absorption
spectroscopy, providing redshifts, column densities and metallicities
for galaxies far too faint to be accessible directly with current
technology. We have already obtained deep ground based observations for
many hosts and here propose ACS/WFC3 and WFC3 observations of the fields
of bursts at z>3 which are undetected in deep ground based images. These
observations will study the hosts in emission, providing luminosities
and morphologies and will enable the construction of a sample of high-z
galaxies with more detailed physical properties than has ever been
possible before.
STIS/CCD 11845
CCD Dark Monitor Part 2
Monitor the darks for the STIS CCD.
STIS/CCD 11847
CCD Bias Monitor-Part 2
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.
STIS/CCD/MA 11668
Cosmo-chronometry and Elemental Abundance Distribution of the Ancient
Star HE1523-0901
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.
STIS/CCD/MA1 11737
The Distance Dependence of the Interstellar N/O Abundance Ratio: A Gould
Belt Influence?
The degree of elemental abundance homogeneity in the interstellar medium
is a function of the enrichment and mixing processes that govern
galactic chemical evolution. Observations of young stars and the
interstellar gas within ~500 pc of the Sun have revealed a local ISM
that is so well-mixed it is having an impact on ideas regarding the
formation of extrasolar planets. However, the situation just beyond the
local ISM is not so clear. Sensitive UV absorption line measurements
have recently revealed a pattern of inhomogeneities in the interstellar
O, N, and Kr gas-phase abundances at distances of ~500 pc and beyond
that appear nucleosynthetic in origin rather than due to dust depletion.
In particular, based on a sample of 13 sightlines, Knauth et al. (2006)
have found that the nearby stars (d < 500 pc) exhibit a mean
interstellar N/O abundance ratio that is significantly higher (0.18 dex)
than that toward the more distant stars. Interestingly, all of their
sightlines lie in the sky vicinity of the Gould Belt of OB associations,
molecular clouds, and diffuse gas encircling the Sun at a distance of
~400 pc. Is it possible that mixing processes have not yet smoothed out
the recent ISM enrichment by massive stars in the young Belt region? By
measuring the interstellar N/O ratios in a strategic new sample of
sightlines with STIS, we propose to test the apparent N/O homogeneity
inside the Gould Belt and determine if the apparent decline in the N/O
ratio with distance is robust and associated with the Belt region.
STIS/MA1/MA2 11857
STIS Cycle 17 MAMA Dark Monitor
This proposal monitors the behavior of the dark current in each of the
MAMA detectors.
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.
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.
WFC3/IR 12265
Determining the Physical Nature of a Unique Giant Lya Emitter at z=6.595
We propose deep WFC3/IR imaging for a giant Lya emitter (LAE) with a
Keck spectroscopic redshift of z=6.595 discovered by extensive
narrow-band imaging with Subaru in the SXDS-UKIDSS/UDS field. This
remarkable object is unique in many respects including its large stellar
mass and luminous nebula which extends over 17 kpc; no equivalent source
has been found in other surveys. The nature of this rare object is
unclear. Fundamental to progress is determining the origin of star
formation in such an early massive object; if the age of the stellar
population is short we are likely witnessing a special moment in the
formation history of a massive galaxy. The heating source for the nebula
is also unclear; options include intense star formation, the infall of
cold gas onto a dark halo or shock heating from a merger. We will take
deep broad-band (F125W and F160W) images and an intermediate-band
(F098M) image which will be analyzed in conjunction with ultra-deep IRAC
3.6 and 4.5 micron data being taken by the Spitzer/SEDS project. These
data will enable us to constrain the star formation rate and stellar
age. Moreover, the UV continuum morphology and Lya-line distribution
will be investigated for evidence of a major merger, cold accretion, or
hot bubbles associated with outflows. We will address the physical
origin of the remarkable object observed at an epoch where massive
galaxies are thought to begin their assembly.
WFC3/IR/S/C 11929
IR Dark Current Monitor
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).
WFC3/UVIS 11905
WFC3 UVIS CCD Daily Monitor
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).
WFC3/UVIS 11914
UVIS Earth Flats
This program is an experimental path finder for Cycle 18 calibration.
Visible-wavelength flat fields will be obtained by observing the dark
side of the Earth during periods of full moon illumination. The
observations will consist of full-frame streaked WFC3 UVIS imagery: per
22- min total exposure time in a single "dark-sky" orbit, we anticipate
collecting 7000 e/pix in F606W or 4500 e/pix in F814W. To achieve
Poisson S/N > 100 per pixel, we require at least 2 orbits of F606W and 3
orbits of F814W.
For UVIS narrowband filters, exposures of 1 sec typically do not
saturate on the sunlit Earth, so we will take sunlit Earth flats for
three of the more-commonly used narrowband filters in Cycle 17 plus the
also-popular long-wavelength quad filters, for which we get four filters
at once.
Why not use the Sunlit Earth for the wideband visible-light filters? It
is too bright in the visible for WFC3 UVIS minimum exposure time of 0.5
sec. Similarly, for NICMOS the sunlit-Earth is too bright which
saturates the detector too quickly and/or induces abnormal behaviors
such as super-shading (Gilmore 1998, NIC 098-011). In the narrowband
visible and broadband near- UV is not too bright (predictions in Cox et
al. 1987 "Standard Astronomical Sources for HST: 6. Spatially Flat
Fields." and observations in ACS Program 10050).
Other possibilities? Cox et al.'s Section II.D addresses many other
possible sources for flat fields, rejecting them for a variety of
reasons. A remaining possibility would be the totally eclipsed moon.
Such eclipses provide approximately 2 hours (1 HST orbit) of opportunity
per year, so they are too rare to be generically useful. An advantage of
the moon over the Earth is that the moon subtends less than 0.25 square
degree, whereas the Earth subtends a steradian or more, so scattered
light and light potentially leaking around the shutter presents
additional problems for the Earth. Also, we're unsure if HST can point
180 deg from the Sun.
WFC3/UVIS/IR 11909
UVIS Hot Pixel Anneal
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.
David Cottle
UBB Owner & Administrator
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