HUBBLE
SPACE TELESCOPE - Continuing to Collect World Class Science
DAILY
REPORT #5104
PERIOD
COVERED: 5am May 25 - 5am May 26, 2010 (DOY 145/09:00z-146/09:00z)
FLIGHT
OPERATIONS SUMMARY:
Significant
Spacecraft Anomalies: (The following are preliminary reports
of
potential non-nominal performance that will be investigated.)
HSTARS:
(None)
COMPLETED
OPS REQUEST: (None)
COMPLETED
OPS NOTES: (None)
SCHEDULED SUCCESSFUL
FGS
GSAcq
06
06
FGS
REAcq 09
09
OBAD
with Maneuver 05 05
SIGNIFICANT
EVENTS: (None)
OBSERVATIONS
SCHEDULED:
ACS/WFC
11995
CCD
Daily Monitor (Part 2)
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 320 orbits (20 weeks) from 1 February 2010 to 20 June
2010.
COS/FUV
11895
FUV
Detector Dark Monitor
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.
COS/FUV/COS/NUV
11579
The
Difference Between Neutral- and Ionized-Gas Metal Abundances in
Local
Star-Forming Galaxies with COS
The
metallicity of galaxies and its evolution with redshift is of
paramount
importance for understanding galaxy formation. Abundances in
the
interstellar medium (ISM) are typically determined using
emission-line
spectroscopy of HII regions. However, since HII regions
are
associated with recent SF they may not have abundances typical for
the
galaxy as a whole. This is true in particular for star-forming
galaxies
(SFGs), in which the bulk of the metals may be contained in the
neutral
gas. It is therefore important to directly probe the metal
abundances
in the neutral gas. This can be done using absorption lines
in
the Far UV. We have developed techniques to do this in SFGs, where
the
absorption is measured for sightlines toward bright SF regions
within
the galaxy itself. We have successfully applied this technique to
a
sample of galaxies observed with FUSE. The results have been very
promising,
suggesting in I Zw 18 that abundances in the neutral gas may
be
up to 0.5 dex lower than in the ionized gas. However, the
interpretation
of the FUSE data is complicated by the very large FUSE
aperture
(30 arcsec), the modest S/N, and the limited selection of
species
available in the FUSE bandpass. The advent of COS on HST now
allows
a significant advance in all of these areas. We will therefore
obtain
absorption line spectroscopy with G130M in the same sample for
which
we already have crude constraints from FUSE. We will obtain
ACS/SBC
images to select the few optimal sightlines to target in each
galaxy.
The results will be interpreted through line-profile fitting to
determine
the metal abundances constrained by the available lines. The
results
will provide important new insights into the metallicities of
galaxies,
and into outstanding problems at high redshift such as the
observed
offset between the metallicities of Lyman Break Galaxies and
Damped
Lyman Alpha systems.
COS/FUV/COS/NUV
11601
UV
spectroscopy of the hot bare stellar core H1504+65
H1504+65
is the hottest known white dwarf (Teff=200, 000 K). It has an
extraordinary
surface composition. The surface is devoid of hydrogen and
helium.
It is mainly composed of carbon and oxygen (by equal amounts)
and
neon (2%). We obviously see the exposed core of a former red giant.
The
evolutionary history of this unique object is unknown. We have
identified
magnesium absorption lines in the soft X-ray photospheric
Chandra
spectrum, which suggests that H1504+65 may be an O-Ne-Mg white
dwarf.
We will test this hypothesis by abundance determinations of Mg
and
Na. If confirmed, then H1504+65 would be the most compelling case
for
the existence of single O-Ne-Mg white dwarfs.
COS/FUV/COS/NUV
11741
Probing
Warm-Hot Intergalactic Gas at 0.5 < z < 1.3 with a Blind Survey
for
O VI, Ne VIII, Mg X, and Si XII Absorption Systems
Currently
we can only account for half of the baryons (or less) expected
to
be found in the nearby universe based on D/H and CMB observations.
This
"missing baryons problem" is one of the highest-priority challenges
in
observational extragalatic astronomy. Cosmological simulations
suggest
that the baryons are hidden in low-density, shock-heated
intergalactic
gas in the log T = 5 - 7 range, but intensive UV and X-ray
surveys
using O VI, O VII, and O VIII absorption lines have not yet
confirmed
this prediction. We propose to use COS to carry out a
sensitive
survey for Ne VIII and Mg X absorption in the spectra of nine
QSOs
at z(QSO) > 0.89. For the three highest-redshift QSOs, we will also
search
for Si XII. This survey will provide more robust constraints on
the
quantity of baryons in warm-hot intergalactic gas at 0.5 < z < 1.3,
and
the data will provide rich constraints on the metal enrichment,
physical
conditions, and nature of a wide variety of QSO absorbers in
addition
to the warm-hot systems. By comparing the results to other
surveys
at lower redshifts (with STIS, FUSE, and from the COS GTO
programs),
the project will also enable the first study of how these
absorbers
evolve with redshift at z < 1. By combining the program with
follow-up
galaxy redshift surveys, we will also push the study of
galaxy-absorber
relationships to higher redshifts, with an emphasis on
the
distribution of the WHIM with respect to the large-scale matter
distribution
of the universe..
COS/NUV
11520
COS-GTO:
QSO Absorbers, Galaxies and Large-scale Structures in the Local
Universe.
This
is a program to probe the large scale structure of baryons in the
universe,
including addressing questions of baryon fraction, physical
conditions
and relationships between absorbers and large-scale
structures
of galaxies. Besides these specific goals, this proposed GTO
program
also probes a large enough total path length in Ly alpha and OVI
to
add significantly to what STIS/FUSE has already observed. Several
Galactic
High Velocity Cloud Complexes also are probed by these
sightlines,
particularly the M Complex. The total path length of this
proposed
program for Ly alpha large-scale structure surveys is
delta_z~5.5.
We
have selected a variety of targets to address these questions, under
the
following subcategories:
1.
Target 8 bright BL Lac objects to search for low contrast Ly alpha
absorbers
from the warm-hot interstellar medium (WHIM). Science drivers:
What
are physical conditions and extent of warm-hot IGM in the current
epoch?
Can we discover metal-poor WHIM using very broad Ly alpha lines?
What
is the number density of such lines (dN/dz) and what is their
relationship
if any with tentative Chandra detections of even hotter
gas?
2.
Ly alpha cloud sizes: The targets are a bright AGN pair which yield
tangential
distance separations of 100--500 kpc at z=0.01--0.05, where
galaxy
surveys are excellent. This pair has two filaments and two voids
in
this distance range. Science drivers: What are the characteristic
sizes
of Ly alpha absorbers, weak metal-line absorbers and absorbers in
voids?
Better size determinations will tighten current estimates of the
baryon
content of the photoionzed IGM .
3.
Probes of starburst outflows: The targets are bright AGN, <= 100 kpc
in
projection out of the minor axis of nearby starburst galaxies.
Science
drivers: Outflowing, unbound winds have been implicated as a
primary
mechanism to enrich the IGM in mass, metals and energy. But do
starburst
winds from massive galaxies escape the galaxy's gravitational
potential?
If so, what is the metallicity and what are mass outflow
rates
of these winds?
4.
A large galaxy's gaseous halo: Three probes of the kinematics and
metallicity
of a single L* galaxy halo. These observations includes
G130M,
G160M exposures at SNR~20 and G285M at 2850A and SNR~10 for MgII.
The
2L* galaxy, ESO 157-G049 (cz=1678 km/s), being probed by these
sightlines
has an available H I 21cm map from ATCA, H alpha imaging from
CTIO
and long-slit spectra from MSSSO. Science drivers: What are the
extent,
metallicity, ionization conditions and kinematics of gaseous
halos
of normal luminous (L*) galaxies? Is there evidence for outflow,
inflow
or galactic fountain circulation of gas in massive galaxy halos?
What
is the source of halo gas (outflowing winds, infalling metal-poor
gas
from stripping of nearby dwarf galaxies, nuclear outflows, large
numbers
of bound dark matter halos??) and what is the relationship
between
this gas and Galactic high-velocity clouds (HVCs)?
5.
Dwarf galaxy
COS/NUV
11894
NUV
Detector Dark Monitor
Measure
the NUV detector dark rate by taking long science exposures with
no
light on 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.
S/C/WFC3/IR
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).
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
11855
STIS/CCD
Spectroscopic Sensitivity Monitor for Cycle 17
Monitor
sensitivity of each CCD grating mode to detect any change due to
contamination
or other causes.
WFC3/IR
11702
Search
for Very High-z Galaxies with WFC3 Pure Parallel
WFC3
will provide an unprecedented probe to the early universe beyond
the
current redshift frontier. Here we propose a pure parallel program
using
this new instrument to search for Lyman-break galaxies at
6.5<z<8.8
and to probe the epoch of reionization, a hallmark event in
the
history of the early universe. We request 200 orbits, spreading over
30
~ 50 high Galactic latitude visits (|b|>20deg) that last for 4 orbits
and
longer, resulting a total survey area of about 140~230 square
arcminute.
Based on our understanding of the new HST parallel
observation
scheduling process, we believe that the total number of
long-duration
pure parallel visits in Cycle 17 should be sufficient to
accommodate
our program. We waive all proprietary rights to our data,
and
will also make the enhanced data products public in a timely manner.
(1)
We will use both the UVIS and the IR channels, and do not need to
seek
optical data from elsewhere. (2) Our program will likely triple the
size
of the probable candidate samples at z~7 and z~8, and will
complement
other targeted programs aiming at the similar redshift range.
(3)
Being a pure parallel program, our survey will only make very
limited
demand on the scarce HST resources. More importantly, as the
pure
parallel pointings will be at random sight-lines, our program will
be
least affected by the bias due to the large scale structure ("cosmic
variance").
(4) We aim at the most luminous LBG population, and will
address
the bright-end of the luminosity function at z~8 and z~7. We
will
constrain the value of L* in particular, which is critical for
understanding
the star formation process and the stellar mass assembly
history
in the first few hundred million years of the universe. (5) The
candidates
from our survey, most of which will be the brightest ones
that
any surveys would be able to find, will have the best chance to be
spectroscopically
confirmed at the current 8--10m telescopes. (6) We
will
also find a large number of extremely red, old galaxies at
intermediate
redshifts, and the fine spatial resolution offered by the
WFC3
will enable us constrain their formation history based on the study
of
their morphology, and hence shed light on their connection to the
very
early galaxies in the universe.
WFC3/IR
11712
Calibration
of Surface Brightness Fluctuations for WFC3/IR
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
characterisitics
(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.
WFC3/UVI
11702
Search
for Very High-z Galaxies with WFC3 Pure Parallel
WFC3
will provide an unprecedented probe to the early universe beyond
the
current redshift frontier. Here we propose a pure parallel program
using
this new instrument to search for Lyman-break galaxies at
6.5<z<8.8
and to probe the epoch of reionization, a hallmark event in
the
history of the early universe. We request 200 orbits, spreading over
30
~ 50 high Galactic latitude visits (|b|>20deg) that last for 4 orbits
and
longer, resulting a total survey area of about 140~230 square
arcminute.
Based on our understanding of the new HST parallel
observation
scheduling process, we believe that the total number of
long-duration
pure parallel visits in Cycle 17 should be sufficient to
accommodate
our program. We waive all proprietary rights to our data,
and
will also make the enhanced data products public in a timely manner.
(1)
We will use both the UVIS and the IR channels, and do not need to
seek
optical data from elsewhere. (2) Our program will likely triple the
size
of the probable candidate samples at z~7 and z~8, and will
complement
other targeted programs aiming at the similar redshift range.
(3)
Being a pure parallel program, our survey will only make very
limited
demand on the scarce HST resources. More importantly, as the
pure
parallel pointings will be at random sight-lines, our program will
be
least affected by the bias due to the large scale structure ("cosmic
variance").
(4) We aim at the most luminous LBG population, and will
address
the bright-end of the luminosity function at z~8 and z~7. We
will
constrain the value of L* in particular, which is critical for
understanding
the star formation process and the stellar mass assembly
history
in the first few hundred million years of the universe. (5) The
candidates
from our survey, most of which will be the brightest ones
that
any surveys would be able to find, will have the best chance to be
spectroscopically
confirmed at the current 8--10m telescopes. (6) We
will
also find a large number of extremely red, old galaxies at
intermediate
redshifts, and the fine spatial resolution offered by the
WFC3
will enable us constrain their formation history based on the study
of
their morphology, and hence shed light on their connection to the
very
early galaxies in the universe.
WFC3/UVI
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<BR>and dark frames. A smaller set of 2Kx4K
subarray
biases are acquired at less frequent intervals<BR>throughout
the
cycle to support subarray science observations. The internals from
this
proposal,<BR>along with those from the anneal procedure (11909),
will
be used to generate the necessary superbias<BR>and superdark
reference
files for the calibration pipeline (CDBS).
WFC3/UVI
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 ~20C. 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.