Status Report

Hubble Space Telescope Daily Report #3176 – 12 Aug 2002

By SpaceRef Editor
August 12, 2002
Filed under , ,
HUBBLE SPACE TELESCOPE

DAILY REPORT # 3176

PERIOD COVERED: DOY 221-223

OBSERVATIONS SCHEDULED (see HSTARS below for possible observation problems)

WFPC2 9676

POMS Test Proposal: WFII parallel archive proposal

This is the generic target version of the WFPC2 Archival Pure Parallel
program.
The program will be used to take parallel images of random areas of the sky,
following the recommendations of the 2002 Parallels Working Group.

ACS 9472

A Snapshot Survey for Gravitational Lenses among z >= 4.0 Quasars

Over the last few years, the Sloan Digital Sky Survey has revolutionized the
study of high-redshift quasars by discovering over 200 objects with redshift
greater than 4.0, more than doubling the number known in this redshift
interval.
The sample includes eight of the ten highest redshift quasars known. We
propose
a snapshot imaging survey of a well-defined sample of 250 z > 4.0 quasars in
order to find objects which are gravitationally lensed. Lensing models
including
magnification bias predict that at least 4% of quasars in a flux-limited
sample
at z > 4 will be multiply lensed. Therefore this survey should find of order
10
lensed quasars at high redshift; only one gravitationally lensed quasar is
currently known at z > 4. This survey will provide by far the best sample to
date of high-redshift gravitational lenses. The observed fraction of lenses
can
put strong constraints on cosmological models, in particular on the
cosmological
constant Lambda. In addition, magnification bias can significantly bias
estimates of the luminosity function of quasars and the evolution thereof;
this
work will constrain how important an effect this is, and thereby give us a
better understanding of the evolution of quasars and black holes at early
epochs, as well as constrain models for black hole formation.

ACS 9480

Cosmic Shear With ACS Pure Parallels

Small distortions in the shapes of background galaxies by foreground mass
provide a powerful method of directly measuring the amount and distribution
of
dark matter. Several groups have recently detected this weak lensing by
large-scale structure, also called cosmic shear. The high resolution and
sensitivity of HST/ACS provide a unique opportunity to measure cosmic shear
accurately on small scales. Using 260 parallel orbits in Sloan textiti
{F775W}
we will measure for the first time: beginlistosetlength sep0cm
setlengthemsep0cm
setlength opsep0cm em the cosmic shear variance on scales <0.7 arcmin, em
the
skewness of the shear distribution, and em the magnification effect.
endlist Our
measurements will determine the amplitude of the mass power spectrum
sigma_8Omega_m^0.5, with signal-to-noise {s/n} ~ 20, and the mass density
Omega_m with s/n=4. They will be done at small angular scales where
non-linear
effects dominate the power spectrum, providing a test of the gravitational
instability paradigm for structure formation. Measurements on these scales
are
not possible from the ground, because of the systematic effects induced by
PSF
smearing from seeing. Having many independent lines of sight reduces the
uncertainty due to cosmic variance, making parallel observations ideal.

ACS 9665

Extreme Red Stars

ACS provides unprecedented sensitivity in the far red, this coupled with
recent
astronomical pushes to ever cooler objects {e.g. new classifications for L
and T
stellar dwarfs, and extremely high redshift galaxies} increases the need for
extending the photometric calibration to include such objects. We propose
observations of 4 stellar objects for which excellent ground based optical
and
near-IR data exist that span V-I colors of 4.5 at M7 to > 6.0 at L5.

ACS 9395

Is Bulge Formation Still Going-On? An ACS Survey of Pseudo-Bulges

Pseudo-bulges, i.e., bulges with an exponential light profile, have been
unveiled in the centers of many intermediate-type disks. Their structural
similarity with the disks provides support to theoretical scenarios in which
bulges may form due to secular evolution processes within the host disks. If
at
play, these processes would likely be active throughout a large fraction of
cosmic history down to our days: `young' bulges should exist. Our previous
HST
WFPC2 and NICMOS survey of ~100 spirals has provided V-H colors for 11 Sb-Sc
pseudo-bulges, and these could be interpreted as suggestive of relatively
young
stellar ages. Furthermore, dense nuclei have been discovered in these
pseudo-bulges, and their V-H colors may imply stellar masses sufficiently
large
to activate the formation of the pseudo- bulge by means of dynamical
dissolution
of progenitor bars. However, the V-H color, on its own, is fully degenerate
towards stellar ages, metallicities and masses, as well as dust content. We
therefore propose to use ACS to observe the 11 pseudo-bulges of our combined
WFPC2 and NICMOS sample in the F330W, F435W, and F814W filters. Extending
the
wavelength baseline to the bluer passbands is essential to break the
mass-age-metallicity-dust degeneracy, and will provide far more accurate
estimates for the stellar population properties of the pseudo-bulges and
their
nuclei. Proving the existence of `young' bulges in the local Universe would
have
a big impact in our understanding of the formation of the Hubble sequence.

ACS 9563

Preliminary ACS Sensitivity

A spectrophotometric standard star is observed through a popular subset of
filters of each camera to assess the sensitivity of the instrument. The star
is
placed at the centre of the aperture, and two images are taken through each
filter. This programme is based on proposal 9020 designed for SMOV. There
are
three groups of visits, numbered respectively 1 through 3, 4 through 6 and 7
through 9. The three visits in each group must be executed about one month
apart
from one another, as indicated in the visit requirements. The first visit in
each group {namely visits 1, 4 and 7} ought to be scheduled during the month
of
July 2002. During SMOV the standard star GD71 could be used, which is not
visible during the Cycle 11 interim calibration period. We have selected
GRW+705824 instead. The latter is a WD slightly brighter than GD71 in V but
with
very similar spectral properties. The exposure times with this object have
been
selected to reach, on average, SNR~350 in the central pixel for broad band
filters.

ACS 9425

The Great Observatories Origins Deep Survey: Imaging with ACS

We propose a Treasury program of ACS imaging as part of the Great
Observatories
Origins Deep Survey {GOODS}, covering 320{square}', or 32* the area of the
two
original WFPC2 HDFs, to within 0.5--0.8 mag of their depth in four ACS
bands,
BViz. The two GOODS fields, the Hubble Deep Field North and Chandra Deep
Field
South, are the premier deep survey areas from X-- ray to radio wavelengths.
ACS
data will provide unique angular resolution, sensitivity, and wavelength
coverage to close the gap between the deepest Chandra and SIRTF
observations.
Supported by extensive imaging and spectroscopy from the VLT, Keck, Subaru,
NOAO, Gemini, VLA, JCMT, and other facilities, the combined GOODS data set
will
make it possible to map the evolution of the Hubble sequence with redshift,
reconstruct the history of galaxy mass assembly, star formation and nuclear
activity from the epoch of reionization to the present, trace the growth of
density perturbations via cosmic shear, and, with properly phased z--band
observations, detect ~ 12 Type Ia supernovae at 1.2<z<1.8 to test the cosmic
acceleration and the presence of dark energy. All HST, SIRTF, Chandra, and
supporting GOODS data are non-- proprietary, with science--quality images
and
catalogs released on a timescale of months. This will constitute the
deepest,
largest, and most uniform panchromatic data set ever assembled to study the
distant universe.

ACS 9396

Young Cluster Systems in Two Super-Gas- Rich Mergers: Arp 220 and Arp 299

Massive young star clusters are found in large numbers within the mergers of
massive, gas-rich disk galaxies. The most outstanding and well studied case
is
in the nearby merging Antennae pair {Whitmore and colleagues}. These
systems may
give us our best hope to see directly the way in which globular clusters
formed
in the uniquely gas-rich protogalactic era of the universe. But, even in the
Antennae, the many hundreds of young clusters have a median mass which is
still
5 to 10 times smaller than the characteristic mass ~ 3 * 10^5 M_odot that
characterizes normal, old-halo globular clusters. To find objects closer to
the
mass range of ``true'' protoglobular clusters, we need mergers which are
still
more gas-rich than the Antennae and in which the gas has been collected into
more massive GMCs. Two excellent candidates are Arp 220 and Arp 299, both of
which are undergoing extremely high star formation rates and have > 10^10
M_odot
of molecular hydrogen compressed into their central few kpc. With the ACS
High
Resolution Camera we will obtain deep UBVI imaging of the active central
regions
of these galaxies, allowing us to trace the luminosities, colors, masses,
and
ages of the young star clusters within them.

ACS/CAL 9558

ACS weekly Test

This program consists of basic tests to monitor, the read noise, the
development
of hot pixels and test for any source of noise in ACS CCD detectors. This
programme will be executed once a day for the entire lifetime of ACS.

ACS/HRC 9379

Near Ultraviolet Imaging of Seyfert Galaxies: Understanding the
Starburst-AGN
Connection

We propose a near-UV snapshot survey of 101 Seyfert galaxies using ACS/HRC
and
the filter F330W, a configuration which is optimal to detect faint star
forming
regions around their nuclei. These images will complement optical and
near-IR
images available in the HST archive, thus providing a panchromatic atlas of
the
inner regions of active galaxies, which we will use to study the
starburst-AGN
connection. The main goals of this proposal are: {1} Determine the frequency
of
circumnuclear starbursts in Seyferts, down to levels which cannot be
observed
from the ground; {2} characterize the observational {fluxes, colors,
structure,
sizes} and intrinsic {luminosities, masses, ages, global star-formation
rate}
properties of these clusters; {3} derive the luminosity functions of young
star
clusters around the nucleus of Seyferts and compare these results with those
from normal and starburst galaxies to determine their survival rate close
to the
AGN; {4} address questions about the relation between AGNs and starbursts,
like
the possible connection between the masses and luminosities of black holes
and
starbursts, and the implications for the evolution of the black holes and
their
host galaxy bulges. By adding UV images to the existing optical and near-IR
ones, this project will create an extremely valuable database for
astronomers
with a broad range of scientific interests, from the properties of the AGN
to
the properties of their host galaxies.

ACS/WFC/HRC 9562

Cycle 11 Internal Flat Field Stability.

The Advance Camera for Surveys (WFC and HRC) was used to obtain flat field
stability and characterization samples of the ACS filter set. Only internal
exposures using the calibration lamps were required.

ACS/WFPC2 9488

Cosmic Shear - with ACS Pure Parallel Observations

The ACS, with greater sensitivity and sky coverage, will extend our ability
to
measure the weak gravitational lensing of galaxy images caused by the large
scale distribution of dark matter. We propose to use the ACS in pure
parallel
{non- proprietary} mode, following the guidelines of the ACS Default Pure
Parallel Program. Using the HST Medium Deep Survey WFPC2 database we have
measured cosmic shear at arc-min angular scales. The MDS image parameters,
in
particular the galaxy orientations and axis ratios, are such that any
residual
corrections due to errors in the PSF or jitter are much smaller than the
measured signal. This situation is in stark contrast with ground-based
observations. We have also developed a statistical analysis procedure to
derive
unbiased estimates of cosmic shear from a large number of fields, each of
which
has a very small number of galaxies. We have therefore set the stage for
measurements with the ACS at fainter apparent magnitudes and smaller, 10
arc-second scales corresponding to larger cosmological distances. We will
adapt
existing MDS WFPC2 maximum likelihood galaxy image analysis algorithms to
work
with the ACS. The analysis would also yield an online database similar to
that
in archive.stsci.edu/mds/

ACS/WFPC2 9481

Pure Parallel Near-UV Observations with WFPC2 within High-Latitude ACS
Survey
Fields

In anticipation of the allocation of ACS high-latitude imaging survey{s}, we
request a modification of the default pure parallel program for those WFPC2
parallels that fall within the ACS survey field. Rather than duplicate the
red
bands which will be done much better with ACS, we propose to observe in the
near-ultraviolet F300W filter. These data will enable study of the
rest-frame
ultraviolet morphology of galaxies at 0<z<1. We will determine the
morphological
k-correction, and the location of star formation within galaxies, using a
sample
that is likely to be nearly complete with multi-wavelength photometry and
spectroscopic redshifts. The results can be used to interpret observations
of
higher redshift galaxies by ACS.

FGS 9347

FGS Astrometry of the Extrasolar Planet of Epsilon Eridani

We propose observations with HST/FGS in Position Mode to determine the
astrometric elements {perturbation orbit semimajor axis and inclination} of
the
candidate extra-solar planet around the K2 V star Epsilon Eridani that has
been
detected by Dopler spectroscopy. These observations will also permit us to
determine the actual mass of the planet by providing the sin{i} factor
which can
not be determined with the radial velocity method. High precision radial
velocity {RV} measurements spanning the years 1980.8--2000.0 for the nearby
{3.22 pc} star Epsilon Eri show convincing variations with a period of ~ 7
yrs.
These data represent a combination of six independent data sets taken with
four
different telescopes. A least squares orbital solution using robust
estimation
yields orbital parameters of period, P = 6.9 yrs, velocity K- amplitude = 19
m/s, eccentricity e = 0.6, projected companion mass M_B sin{i} = 0.83
M_Jupiter.
An estimate of the inclination yields a perturbation semi-major axis, Alpha
=
0arcs0022, easily within the reach of HST/FGS astrometry.

NICMOS 9386

Infrared Photometry of a Statistically Significant Sample of KBOs

While the discovery rate of Kuiper Belt objects is accelerating, the
physical
study of this new region of the solar system has been slowed by a lack of
basic
astrophysical data. Photometric observations of the majority of the more
than
400 known KBOs and Centaurs are rudimentary and incomplete, particularly in
the
infrared. The multicolor optical-infrared photometry that exists for a small
subset of KBOs often shows significant discrepancies between observations by
different observers. Their intrinsic faintness puts them at the practical
limits
of ground-based systems. In July 2001 we began what will be the largest
uniform
sample of optical photometry of KBOs with a WFPC2 SNAPSHOT program that will
perform accurate photometry at V, R, and I on a sample of up to 150 targets.
We
seek to greatly enhance the value of this survey by obtaining J and H
photometry
on the same sample using NICMOS. Combined optical and infrared broad band
photometry is a far more powerful tool for physical studies than is either
alone. Our sample includes objects that will be observed at thermal infrared
wavelengths by SIRTF and will be used with those data to derive the first
accurate diameters, albedos, and surface properties for a large sample of
KBOs.

NICMOS 8790

NICMOS Post-SAA calibration - CR Persistence Part 1.

A new procedure proposed to alleviate the CR-persistence problem of NICMOS.
Dark
frames will be obtained immediately upon exiting the SAA contour 23, and
every
time a NICMOS exposure is scheduled within 50 minutes of coming out of the
SAA.
The darks will be obtained in parallel in all three NICMOS Cameras. The
POST-SAA
darks will be non-standard reference files available to users with a
USEAFTER
date/time mark.

NICMOS 9484

The NICMOS Parallel Observing Program

We propose to manage the default set of pure parallels with NICMOS. Our
experience with both our GO NICMOS parallel program and the public parallel
NICMOS programs in cycle 7 prepared us to make optimal use of the parallel
opportunities. The NICMOS G141 grism remains the most powerful survey tool
for
HAlpha emission-line galaxies at cosmologically interesting redshifts. It is
particularly well suited to addressing two key uncertainties regarding the
global history of star formation: the peak rate of star formation in the
relatively unexplored but critical 1<= z <= 2 epoch, and the amount of star
formation missing from UV continuum-based estimates due to high extinction.
Our
proposed deep G141 exposures will increase the sample of known HAlpha
emission-
line objects at z ~ 1.3 by roughly an order of magnitude. We will also
obtain a
mix of F110W and F160W images along random sight-lines to examine the space
density and morphologies of the reddest galaxies. The nature of the
extremely
red galaxies remains unclear and our program of imaging and grism
spectroscopy
provides unique information

regarding both the incidence of obscured star bursts and the build up of
stellar
mass at intermediate redshifts. In addition to carrying out the parallel
program
we will populate a public database with calibrated spectra and images, and
provide limited ground- based optical and near-IR data for the deepest
parallel
fields.

POMS 9677

POMS Test Proposal: WFII backup parallel archive proposal

This is a POMS test proposal designed to simulate scientific plans.

SNAP 9356

SNAPSHOT survey of the Planetary Nebulae population of the Galactic Bulge

The spectacular structures seen in HST images of planetary nebulae {PNe} are
generally accepted as originating from hydrodynamical interactions between
stellar winds: the interacting-stellar wind model {ISW}. Traditionally, the
shaping is thought to occur after the star becomes hot enough to ionize the
PN.
But recent HST images indicate that the shaping may occur earlier, and the
newer
GISW model puts the shaping during the pre-planetary nebula evolution. The
relative importance of both models is not known: GISW shaping will account
for
some fraction of PNe, but estimates range from 15--100 during the PN phase,
especially for the youngest PNe. We here propose an HST SNAPshot survey of
compact PNe in the Galactic Bulge, to test these predictions. The Bulge
provides
the only PNe population for which progenitor masses are known and nebular
ages
can be measured. In support of these HST measurements we have already
measured
velocity fields and emission line fluxes. The survey will give an unbiassed
sampling of morphologies, and allow evolutionary sequences to be determined
to
test the ISW versus the GISW model. By-products of the survey will be the
determination of nebular masses, diameters and filling factors. We will also
obtain the White Dwarf mass distribution in the Bulge, and the initial-final
mass function for low-mass stars.

STIS/CCD 8904

Bias Monitor-Part 2.

The Space Telescope Imaging Spectrograph (CCD) was used to monitor the bias
in
the 1x1, 1x2, 2x1, and 2x2 bin settings at gain=1, and 1x1 at gain = 4 in
order
to build up high-S/N superbiases and track the evolution of hot columns.

STIS/CCD 9066

Closing in on the Hydrogen Reionization Edge of the Universe.

The Space Telescope Imaging Spectrograph (CCD) was used in parallel
constrain
the Hydrogen reionization edge in emission that marks the transition from a
neutral to a fully ionized IGM at a predicted redshifts.

STIS/CCD 8902

Dark Monitor-Part 2.

The Space Telescope Imaging Spectrograph (CCD) was used to monitor the
darks.

STIS/CCD 8906

Hot Pixel Annealing.

The Space Telescope Imaging Spectrograph (CCD) was used to measure the
effectiveness of the CCD hot pixel annealing process by measuring the dark
current behavior before and after annealing and by searching for any window
contamination effects. In addition, CTE performance is examined by looking
for
traps in a low signal level flat.

STIS/CCD 8928

PSFs at Pseudo-Apertures {Cycle 10}.

The Space Telescope Imaging Spectrograph (CCD) was used to perform
spectroscopic
PSF measurements, performed for the new pseudo-apertures located near CCD
row
900, which are made available to ameliorate CCD CTE losses.

STIS/CCD 9317

Pure Parallel Imaging Program: Cycle 10.

The Space Telescope Imaging Spectrograph (CCD) was used to perform the
default
archival pure parallel program for STIS during cycle 10.

STIS/CCD/MA2 9166

Fossil Gaseous Halos of Massive Galaxies at z~1.

The Space Telescope Imaging Spectrograph (CCD and MA2) was used to observe
host
galaxies of high-redshift, powerful radio sources that are likely the
progenitors of present-day gE and cD galaxies, and therefore provide
important
laboratories in which to investigate the formation of massive galaxies in
the
early Universe. Many high-redshift radio galaxies exhibit giant, Ly-alpha
halos.
Similar nebulae without associated radio sources have recently been
discovered
in a galaxy overdensity at z = 3.09. The LyAlpha luminosity of these halos
is
comparable to the total X-ray luminosities of low--z X--ray clusters, and
may
reflect the hot, cooling gas reservoir from which the galaxy/cluster is
forming.

WF/PC-2 9091

Evolution of Star Forming Environments in H II Regions.

The WF/PC-2 was used to look for evaporating gaseous globules and silhouette
disks in two young clusters and along one molecular cloud wall.

WFPC2 9393

Dynamics and Cloud Structure of Neptune

A 4-year gap in detailed observation of one of the most active planets in
our
solar system can be ended by our proposed multispectral WFPC2 imaging of
Neptune
over a period of 2 Neptune rotations. Our objectives are {1} mapping the
two-
dimensional distribution of Neptune's discrete cloud features and zonal
bands
with sufficiently dense longitudinal sampling to insure detection of any
Great
Dark Spot, or other major storm system, up to 35degrees N, {2}
characterizing
Neptune's circulation by tracking cloud motions during two densely sampled
half-rotations that ensure reliable target identification, and {4}
characterizing the vertical structure of clouds by imaging with filters that
select varying amounts of Rayleigh scattering and methane absorption and by
capturing their center-to-limb variations during intensely sampled feature
transits. To enhance the characterization of cloud structure we will also
propose coordinated groundbased IRTF and Keck observations,both using
adaptive
optics at near IR wavelengths that provide access to additional strong
methane
and hydrogen absorption bands. The proposed HST observations use the same
filters
as in 1996 and 1998, as well as additional filters, permitting detailed
comparisons with previous observations.

WFPC2 9599

WFPC2 Cycle 11 UV Earth Flats

Monitor flat field stability. This proposal obtains sequences of earth
streak
flats to improve the quality of pipeline flat fields for the WFPC2 UV filter
set. These Earth flats will complement the UV earth flat data obtained
during
cycles 8-10.

WFPC2 8938

WFPC2 CYCLE 9 SUPPLEMENTAL DARKS pt3/3.

This dark calibration program obtains 3 dark frames every day to provide
data
for monitoring and characterizing the evolution of hot pixels.

WFPC2 8934

WFPC2 Decontaminations and Associated Observations Pt. 3/3

This proposal is for the monthly WFPC2 decons. Also included are instrument
monitors tied to decons: photometric stability check, focus monitor, pre-
and
post-decon internals {bias, intflats, kspots, & darks}, UV throughput check,
VISFLAT sweep, and internal UV flat check.

FLIGHT OPERATIONS SUMMARY:

HSTARS (For details see http://hst-sers.hst.nasa.gov/SERS/HST/HSTAR.nsf)

HSTAR 8756: CCS "G" String HSTPS alarming due to a process count of zero
on nascomd.
Under investigation.

HSTAR 8757: NICMOS TPG reset @ 223/04:18:22Z. NICMOS 736, 744, 639, 290,
588, and
two 604 Status Buffer messages received. NICMOS was
in the middle of
Observation 9396 at time of reset.Under investigation.

HSTAR 8758: CCS "G" String Backbone Data Server icon flashing red @
223/07:45Z.
Under investigation.

HSTAR 8759: CCS "B" String can not copy config file from "B" String
(permission denied).
G. Gibson copied the file over for the FOT, they can
now transfer files
from a remote machine. Under investigation.

HSTAR 8760: - Wing Panel Temperature (B_WPANLT) flagged yellow low
(-81.2765 ?C) for
42 seconds (7 samples) @ 223/20:42:50Z. Limit is
-80.0 ?C.Under investigation.

COMPLETED OPS REQs:
16817-0 - FN format to cover acquisitions and reacquisitions in SA217 SMS @
223/1811z

OPS NOTES EXECUTED: None

SCHEDULED SUCCESSFUL FAILURE TIMES
FGS GSacq 20 20
FGS REacq 26 26
FHST Update 47 47
LOSS of LOCK

SIGNIFICANT EVENTS:

NICMOS experienced TPG, Detector 3 reset @ 223/04:18:22Z; similar to one
that
occurred on Day 213. Unlike Day 213, NICMOS was observing on the detector
that experienced the reset, effecting 895 second multi-accumulator exposure
on Camera 3 which started at 223/04:12Z (Proposal 9484). Five Status Buffer
messages were issued, first two were the result of the TPG reset, indicating
OOL condition and a TPG reset on Camera 3, respectively. NICMOS camera was
successfully recovered by SPC and subsequent observations executed as
expected.

HST On-Orbit Checkout of real-time WSC interface scheduled daily 224 - 231
with
GDOC, STOCC Ops (SIMOR), HITT, and CCS using CCS "G" String with CCS
Release 4.0.1
and PRD D06100R2. The purpose of this testing is to verify CCS Release
4.0.1 (IP)
capability to interface through the IP Packet Filters to WSC for real-time
telemetry
and commands.

SpaceRef staff editor.