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============================================================================== TOPIC: Daily Report #5068
== 1 of 1 == Date: Tues, Apr 6 2010 9:59 am From: "Cooper, Joe"
HUBBLE SPACE TELESCOPE - Continuing to Collect World Class Science
DAILY REPORT #5068
PERIOD COVERED: 5am April 5 - 5am April 6, 2010 (DOY 095/09:00z-096/09:00z)
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
ACS/WFC3 11599
Distances of Planetary Nebulae from SNAPshots of Resolved Companions
Reliable distances to individual planetary nebulae (PNe) in the Milky Way are needed to advance our understanding of their spatial distribution, birthrates, influence on galactic chemistry, and the luminosities and evolutionary states of their central stars (CSPN) Few PNe have good distances, however One of the best ways to remedy this problem is to find resolved physical companions to the CSPN and measure their distances by photometric main-sequence fitting We have previously used HST to identify and measure probable companions to 10 CSPN, based on angular separations and statistical arguments only We now propose to use HST to re-observe 48 PNe from that program for which additional companions are possibly present We then can use the added criterion of common proper motion to confirm our original candidate companions and identify new ones in cases that could not confidently be studied before We will image the region around each CSPN in the V and I bands, and in some cases in the B band Field stars that appear close to the CSPN by chance will be revealed by their relative proper motion during the 13+ years since our original survey, leaving only genuine physical companions in our improved and enlarged sample This study will increase the number of Galactic PNe with reliable distances by 50 percent and improve the distances to PNe with previously known companions
COS/FUV 11895
FUV Detector Dark Monitor
The purpose of this proposal is to 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/NUV 11894
NUV Detector Dark Monitor
The purpose of this proposal is to 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
COS/NUV 11896
NUV Spectroscopic Sensitivity Monitoring
The purpose of this proposal is to monitor sensitivity of each NUV grating mode to detect any changes due to contamination or other causes
S/C 12046
COS FUV DCE Memory Dump
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
In the case of a HV transient (known as a "crackle" 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 "mini-crackle" 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 "mini-crackles" and thus learn something about the state of the detector
STIS/CC 11845
CCD Dark Monitor Part 2
Monitor the darks for the STIS CCD
STIS/CC 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 11852
STIS CCD Spectroscopic Flats C17
The purpose of this proposal is to obtain pixel-to-pixel lamp flat fields for the STIS CCD in spectroscopic mode
STIS/CCD 11853
Cycle 17 STIS CCD Imaging Flats
This program periodically monitors the STIS CCD imaging mode flat fields by using the tungsten lamps
STIS/CCD/MA2 11568
A SNAPSHOT Survey of the Local Interstellar Medium: New NUV Observations of Stars with Archived FUV Observations
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
WFC3/UV 11635
Improve the Measurement of Vesta's Pole Orientation to Support Dawn Mission
NASA?s Dawn spacecraft is scheduled to go into orbit around the main belt asteroid 4 Vesta in July 2011 Currently the project is using a 3-? pole position uncertainty of Vesta of 12? for spacecraft trajectory design We have determined that with an additional set of Hubble observations at Vesta?s next opposition in February 2010, that the pole position uncertainty can be reduced by a factor of 4 This will reduce both cost and risk to the Dawn mission, and is likely to increase the stay time at Vesta and will add to the scientific return of the mission The requested observing window in February 2010 is the last and single best opportunity that can benefit the Dawn mission, but it is before the start of the next HST Cycle
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)
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 9 9 FGS REAcq 5 5 OBAD with Maneuver 4 4
SIGNIFICANT EVENTS: (None)
============================================================================== TOPIC: Daily Rpt #5069
== 1 of 1 == Date: Wed, Apr 7 2010 7:58 am From: "Bassford, Lynn"
HUBBLE SPACE TELESCOPE - Continuing to Collect World Class Science
DAILY REPORT #5069
PERIOD COVERED: 5am April 6 - 5am April 7, 2010 (DOY 096/09:00z-097/09:00z)
OBSERVATIONS SCHEDULED
ACS/WFC 11715
The Luminous Galactic Cepheid RS Puppis: A Geometric Distance from its Nested Light Echoes
RS Puppis is one of the most luminous Cepheids in the Milky Way (P = 41 4 days) and an analog of the bright Cepheids used to measure extragalactic distances An accurate distance would help anchor the zero-point of the bright end of the period-luminosity relation, but at a distance of about 2 kpc it is too far away for a trigonometric parallax with existing instrumentation
RS Pup is unique in being surrounded by a reflection nebula, whose brightness varies as pulses of light from the Cepheid propagate outwards Members of our team have used ground-based imaging of the nebula to derive phase lags in the light variations of individual features in the nebula, and have inferred a seemingly very precise geometric distance to the star However, there is an unavoidable ambiguity involving the cycle counts, which was resolved by assuming that the features lie in the plane of the sky If this assumption is incorrect, a large systematic error would be introduced into the distance measurement
We show that polarimetric imaging using the high spatial resolution of ACS/WFC and its ability to image close to the star can resolve this ambiguity and yield a reliable geometric distance to RS Pup We will also obtain a wide-field multicolor image of the nebula, in order to study its morphology and the mass-loss history of the Cepheid
COS/NUV/FUV 11673
Dynamics in the Atmosphere of the Evaporating Planet HD189733b
With HST/STIS, we detected and characterized the upper atmosphere of the extrasolar planet HD209458b, showing that the planet must be evaporating at a rate of ~10^10 g/s in a "blow-off" mechanism
More recently, using ACS we concluded that HD189733b is also evaporating However, because of the low resolution of the ACS prism spectroscopy, the escape rate and mechanism are still to be determined This is one of the prime objectives of the present proposal
COS observations of the absorption line profile with 15 km/s resolution will allow us to probe the dynamics of the escaping gas, and therefore to determine the escape rate Simultaneous observations of the transit depth and spectral shape in several important lines (not only HI, but also OI, CII and possibly NI) will constrain the escape mechanism and allow us to distinguish between several scenarios The results will enlighten the physical phenomenons at work in the exosphere of these extrasolar planets, and provide new constraints for the modeling of the evaporation of hot-Jupiters
STIS/CC 11845
CCD Dark Monitor Part 2
Monitor the darks for the STIS CCD
STIS/CC 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
WFC3/ACS/IR 11142
Revealing the Physical Nature of Infrared Luminous Galaxies at
0
3 We aim to determine physical properties of IR luminous galaxies at
0
3 WFC3/ACS/UVIS 11877 HST Cycle 17 and Post-SM4 Optical Monitor This program is the Cycle 17 implementation of the HST Optical
Monitoring Program
The 36 orbits comprising this proposal will utilize ACS (Wide Field
Channel) and WFC3 (UVIS Channel) to observe stellar cluster members in
parallel with multiple exposures over an orbit
Phase retrieval
performed on the PSF in each image will be used to measure primarily
focus, with the ability to explore apparent coma, and astigmatism
changes in WFC3
The goals of this program are to: 1) monitor the overall OTA focal
length for the purposes of maintaining focus within science tolerances
2) gain experience with the relative effectiveness of phase retrieval
on WFC3/UVIS PSFs 3) determine focus offset between the imagers and
identify any SI-specific focus behavior and dependencies If need is determined, future visits will be modified to interleave
WFC3/IR channel and STIS/CCD focii measurements
WFC3/IR 11920 WFC3 IR Image Quality The IR imaging performance over the detector will be assessed
periodically (every 4 months) in two passbands to check for image
stability
The field around star 58 in the open cluster NGC188 is the
chosen target because it is sufficiently dense to provide good
sampling over the FOV while providing enough isolated stars to permit
accurate PSF (point spread function) measurement
It is available
year-round and used previously for ACS image quality assessment
The
field is astrometric, and astrometric guide stars will be used, so
that the plate scale and image orientation may also be determined if
necessary (as in SMOV proposals 11437 and 11443)
Full frame images
will be obtained at each of 4 POSTARG offset positions designed to
improve sampling over the detector in F098M, F105W, and F160W
The
PSFs will be sampled at 4 positions with subpixel shifts in filters
F164N and F127M
This proposal is a periodic repeat (once every 4 months) of the visits
in SMOV proposal 11437 (activity ID WFC3-24)
The data will be
analyzed using the code and techniques described in ISR WFC3 2008-41
(Hartig)
Profiles of encircled energy will be monitored and presented
in an ISR
If an update to the SIAF is needed, (V2, V3) locations of
stars will be obtained from the Flight Ops
Sensors and Calibrations
group at GSFC, the (V2, V3) of the reference pixel and the orientation
of the detector will be determined by the WFC3 group, and the
Telescopes group will update and deliver the SIAF to the PRDB branch
The specific PSF metrics to be examined are encircled energy for
aperture diameter 0
25, 0
37, and 0
60 arcsec, FWHM, and sharpness
(See ISR WFC3 2008-41 tables 2 and 3 and preceding text
) ~20 stars
distributed over the detector will be measured in each exposure for
each filter
The mean, rms, and rms of the mean will be determined for
each metric
The values determined from each of the 4 exposures per
filter within a visit will be compared to each other to see to what
extent they are affected by "breathing"
Values will be compared from
visit to visit, starting with the values obtained during SMOV after
the fine alignment has been performed, to see if the measures of the
compactness of the PSF indicate degradation over time
The analysis
will be repeated for stars on the inner part of the detector and stars
on the outer part of the detector to check for differential
degradation of the PSF
As an example of the analysis, one can examine the sharpness of the
F160W PSF exposures made during thermal vacuum testing (ISR WFC3
2008-41)
To compare two samples, one can define the PSFs on each half
of the detector (lower and upper) as a sample (with 7 and 8 PSFs,
respectively)
The mean, rms, and rms of the mean sharpness are
0
0826, 0
0067, and 0
0027 for one half, and 0
0773, 0
0049, and
0
0019 for the other
The difference of the means is 0
0053 and the
statistical error in that difference is 0
0033, so the difference is
not significant
WFC3/IR 11926 IR Zero Points We will measure and monitor the zeropoints through the IR filters
using observations of the white dwarf standard stars, GD153, GD71 and
GD191B2B and the solar analog standard star, P330E
Data will be taken
monthly during Cycle 17
Observations of the star cluster, NGC 104,
are made twice to check color transformations
We expect an accuracy
of 2% in the wide filter zeropoints relative to the HST photometric
system, and 5% in the medium- and narrow-band filters
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/UV 11635 Improve the Measurement of Vesta's Pole Orientation to Support Dawn
Mission NASA?s Dawn spacecraft is scheduled to go into orbit around the main
belt asteroid 4 Vesta in July 2011
Currently the project is using a
3- pole position uncertainty of Vesta of 12 for spacecraft trajectory
design
We have determined that with an additional set of Hubble
observations at Vesta?s next opposition in February 2010, that the
pole position uncertainty can be reduced by a factor of 4
This will
reduce both cost and risk to the Dawn mission, and is likely to
increase the stay time at Vesta and will add to the scientific return
of the mission
The requested observing window in February 2010 is the
last and single best opportunity that can benefit the Dawn mission,
but it is before the start of the next HST Cycle
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 11908 Cycle 17: UVIS Bowtie Monitor 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
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) FGS GSAcq 7 7
FGS REAcq 10 10
OBAD with Maneuver 7 7 SIGNIFICANT EVENTS: (None) ============================================================================== You received this message because you are subscribed to the Google Groups "sci
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