Status Report

HST Daily Report #3346

By SpaceRef Editor
April 23, 2003
Filed under , ,

HUBBLE SPACE TELESCOPE

DAILY REPORT     #3346

PERIOD COVERED:  DOY 111

OBSERVATIONS SCHEDULED

 NICMOS                         8791

 NICMOS Post-SAA calibration – CR Persistence Part 2

 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. The keyword ‘USEAFTER=date/time’ will also be added to
the header of each POST-SAA DARK
  frame. The keyword must be populated with the time, in addition to the
date, because HST crosses the
 SAA ~8 times per day so each POST-SAA DARK will need to have the
appropriate time specified, for users
 to identify the ones they need. Both the raw and processed
 images will be archived as POST-SAA DARKSs. Generally we expect that all
NICMOS science/calibration
 observations started within 50 minutes of leaving an SAA will need such
maps to remove the CR
 persistence from the science images. Each observation will need its own
CRMAP, as different SAA
 passages leave different imprints on the NICMOS detectors.

 ACS                            9293

 Massive Black Holes in Early Type Galaxies

 3×10^6 Msun < M_BH < 3x10^9 Msun} at the centers of galaxies and the velocity dispersions of their  bulges. However, uncertainties over the exact slope of the correlation still remain, and it is not  known if such a relation extends to black holes of lower and higher masses. The discovery of small {r ~   a few hundred pc}, well defined, dust and gas disks in the nuclei of some active elliptical galaxies  opened a new avenue for measuring central mass distributions. When ionized gas is present, a small  number of high spatial resolution {e.g. STIS} spectra are sufficient to characterize the disk dynamics  and the galaxy's central mass {e.g., M87, M81, NGC 4374}. We propose to use STIS spectroscopy to  measure black hole masses, using gas dynamics, in the centers of several brightest cluster galaxies  {BCGs}, 2 nearby galaxies with low velocity dispersions, and a number of elliptical galaxies known to  harbor small nuclear dust disks. The proposed targets encompass a wide range of black hole masses,  allowing us to fully examine the M_BH -- sigma relationship. We will also obtain H-alpha and continuum  images to fully characterize the gaseous and dust morphology as well as stellar surface profile in the  central regions.

 ACS/WFC                        9351

 Determining Hubble’s Constant from Observations of Cepheids in the Host
Galaxy of SN Ia 1994ae

 We propose to determine the luminosity of the type Ia supernova {SN Ia}
1994ae by observing Cepheids in
  the host spiral galaxy NGC 3370. Modern CCD photometry has yielded an
extremely tight Hubble diagram
 for SNe Ia with a precisely determined intercept {i.e., Delta H_0/H_0} 1
measurement of the true Hubble
  constant is still limited by the calibration. The HST calibration of
all but a few SNe Ia observed to
 date is significantly compromised by the systematics of photographic
photometry and host galaxy
 extinction, as well as by the photometric uncertainties associated with
WFPC2. In contrast, SN 1994ae
 is one of the very best-observed SNe Ia with CCD photometry. The
exquisite B, V, R, and I light curves
 are well-sampled beginning 10 days before maximum brightness, and they
indicate little reddening. From
 our supernova photometry and the current provisional SN Ia calibration
we would find a distance of 30
 +/- 2.1 Mpc, well within the range where ACS can accurately observe
Cepheid light curves and
 distinguish Cepheids from nonvariable stars.

 NICMOS/STIS CCD                9405

 The Origin of Gamma-Ray Bursts

 The rapid and accurate localization of gamma-ray bursts {GRBs} promised
by a working HETE-2 during the
 coming year may well revolutionize our ability to study these enigmatic,
highly luminous transients. We
  propose a program of HST and Chandra observations to capitalize on this
extraordinary opportunity. We
 will perform some of the most stringent tests yet of the standard model,
in which GRBs represent
 collimated relativistic outflows from collapsing massive stars. NICMOS
imaging and STIS CCD
 spectroscopy will detect broad atomic features of supernovae underlying
GRB optical transients, at
 luminosities more than three times fainter than SN 1998bw. UV, optical,
and X-ray spectroscopy will be
 used to study the local ISM around the GRB. Chandra spectroscopy will
investigate whether the GRB X-ray
  lines are from metals freshly ripped from the stellar core by the GRB.
HST and CTIO infra-red imaging
 of the GRBs and their hosts will be used to determine whether `dark’
bursts are the product of
 unusually strong local extinction; imaging studies may for the first
time locate the hosts of `short’
 GRBs. Our early polarimetry and late-time broadband imaging will further
test physical models of the
 relativistic blast wave that produces the bright GRB afterglow, and will
provide unique insight into
 the influence of the GRB environment on the afterglow.

 ACS/NICMOS                     9483

 Origin and Evolution of IR Luminous Galaxies: Are z>=1 Dusty Starbursts
and z=0 ULIRGs the Same?

 Interactions and mergers involving gas-rich galaxies are the main
driving mechanism behind the luminous
  IR galaxy phenomenon. However it is dangerous to extrapolate this model
directly to high redshifts
 because massive spiral progenitors may have been relatively uncommon at
earlier epochs. Mergers and
 interactions involving less massive but more gas-rich progenitors may
have occurred instead. We propose
  to test this hypothesis directly by imaging 12 FIR-selected, dusty
starbursts at z~1 at sub-kpc
 resolution afforded by HST in the rest frame B and I {observed I and H}
bands using ACS and NICMOS.
 While studying higher redshift systems is clearly desirable,
band-shifting and surface brightness
 dimming makes the investigations of tidal features and the nature of
progenitors possible only
 out to z~ 1 {Hibbard & Vacca 1997}. From the morphologies, surface
brightnesses, and color
 distribution, we will determine the physical status of the starburst
hosts, the history of tidal
 interactions/mergers, and the nature of the progenitors. We will also
test for the presence of hidden
 AGNs and for enhanced galaxy number density. Our 12 target galaxies form
a complete sample of known
 ultraluminous and hyperluminous galaxies at 0.7

 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.

 WFPC2                          9592

 WFPC2 CYCLE 11 Standard Darks

 calibration of the CCD dark current rate, and to monitor and
characterize the evolution of hot pixels.
 Over an extended period these data will also provide a monitor of
radiation damage to the CCDs.

 WFPC2                          9594

 WFPC2 CYCLE 11 SUPPLEMENTAL DARKS pt2/3

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

 WFPC2                          9596

 WFPC2 CYCLE 11 INTERNAL MONITOR

 This calibration proposal is the Cycle 11 routine internal monitor for
WFPC2, to be run weekly to
 monitor the health of the cameras. A variety of internal exposures are
obtained in order to provide a
 monitor of the integrity of the CCD camera electronics in both bays
{gain 7 and gain 15}, a test for
 quantum efficiency in the CCDs, and a monitor for possible buildup of
contaminants on the CCD windows.

 STIS                           9606

 CCD Dark Monitor-Part 2

 Monitor the darks for the STIS CCD.

 STIS                           9608

 CCD Bias Monitor – Part 2

 Monitor the bias in the 1×1, 1×2, 2×1, and 2×2 bin settings at gain=1,
and 1×1 at gain = 4, to build up
  high-S/N superbiases and track the evolution of hot columns.

 STIS                           9613

 STIS CCD Spectroscopic Flats C11

 Obtain CCD flats on the STIS CCD in spectroscopic mode.

 STIS                           9615

 Cycle 11 MAMA Dark Monitor

 This test performs the routine monitoring of the MAMA detector dark
noise. This proposal will provide
 the primary means of checking on health of the MAMA detectors systems
through frequent monitoring of
 the background count rate. The purpose is to look for evidence of change
in dark indicative of detector
 problem developing.

 ACS                            9674

 CCD Daily Monitor

 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.

 STIS                           9706

 STIS Pure Parallel Imaging Program: Cycle 10

 This is the default archival pure parallel program for STIS during cycle
10.

 STIS                           9708

 STIS Pure Parallel Imaging Program: Cycle 11

 This is the default archival pure parallel program for STIS during cycle
11.

 WFPC2                          9709

 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 paralell images of random areas of the sky, following the
recommendations of the 2002
 Parallels Working Group.

FLIGHT OPERATIONS SUMMARY:

Significant Spacecraft Anomalies:
(The following are preliminary reports of potential non-nominal
performance that will be investigated.)

HSTARs:
None

COMPLETED OPS REQs:
None

OPS NOTES EXECUTED:
None

                           SCHEDULED     SUCCESSFUL    FAILURE TIMES
FGS GSacq                      9              9             
FGS REacq                     10             10                
FHST Update                   13             13               
LOSS of LOCK                                     

SIGNIFICANT EVENTS: None

SpaceRef staff editor.