0
Assigned ID: 706
----- Attempting Submission 1 (Fri Feb 24 21:06:15 GMT 2012) -----
HST Phase I Proposal 706 (APT.apt) successfully submitted.
----- Attempting Submission 2 (Fri Feb 24 23:36:38 GMT 2012) -----
Removed hold (that I thought I had removed last time)
1637347726
----- Attempting Submission 1 (Tue Jul 10 21:07:49 GMT 2012) -----
----- Attempting Submission 2 (Fri Aug 10 16:21:27 GMT 2012) -----
----- Attempting Submission 3 (Tue Jan 29 04:13:57 GMT 2013) -----
----- Attempting Submission 4 (Wed Jan 30 16:42:32 GMT 2013) -----
----- Attempting Submission 5 (Fri Feb 01 22:06:33 GMT 2013) -----
----- Attempting Submission 6 (Wed Feb 06 18:42:03 GMT 2013) -----
----- Attempting Submission 7 (Mon Mar 11 03:20:10 GMT 2013) -----
----- Attempting Submission 8 (Wed Mar 13 23:42:56 GMT 2013) -----
----- Attempting Submission 9 (Tue Mar 19 17:40:43 GMT 2013) -----
----- Attempting Submission 10 (Wed May 01 18:12:13 GMT 2013) -----
----- Attempting Submission 11 (Tue May 07 17:22:54 GMT 2013) -----
----- Attempting Submission 12 (Sun Aug 18 02:48:22 GMT 2013) -----
Completing the Census of Ultracool Brown Dwarfs in the Solar Neighborhood using HST/WFC3
Despite the spectacular success of wide-field sky surveys (2MASS, SDSS,
and UKIDSS) in uncovering a large population of brown dwarfs in the
solar neighborhood, it was not until the launch of NASA's Wide-field
Infrared Survey Explorer (WISE) that a moderate-size population of
ultracool brown dwarfs (Teff < 700 K), including the new class of Y
dwarfs, was identified. A complete census of the nearby population of
cold brown dwarfs is essential to measuring the low-mass stellar mass
function and the low-mass limit of star formation. With atmospheric
conditions similar to those of giant planets, cold brown dwarfs are also
excellent proxies with which to test the ultracool model atmospheres
that are critical to our understanding of exoplanets. As part of a
larger followup campaign that involves both ground- and space-based
observatories (including Cycle 7 and 8 Spitzer programs and small Cycle
18 and 19 HST programs), we propose a Large GO program to observe twenty
of the coldest brown dwarfs and brown dwarf candidates uncovered by
WISE. These are the brightest representatives of their type over the
entire sky, but they are too dim, J>20, to be characterized from the
ground. WFC3 G102 and G141 grism spectroscopy will be used to derive
accurate classifications and effective temperatures of the targets, and
the direct images required for wavelength calibration will be used to
anchor the astrometric grid of our ground-based adaptive optics parallax
program. HST/WFC3 observations provide a vital link in characterizing
this ultracool brown dwarf population in the immediate Solar
Neighborhood.
Our proposed program consists of obtaining low-resolution near-infrared spectra of the cold brown dwarf candidates listed in Table 1. We will use the WFC3 G141 grism which provides a resolving power of lambda / Delta lambda ~ 130 over the 1.1-1.7 um wavelength range and the G102 grism to cover from 0.8 to 1.15 um at lambda / Delta lambda ~ 210. In order to wavelength calibrate the slitless grism images, direct images of the fields in the F125W and F098M filters will be obtained. We note that the standard G141 direct-image filter is F140W. However the exposure times for the F125W filter are nearly identical and the F125W is a much better match to ground-based J-band filters which facilitates a comparison of the WFC3 photometry to previous work and also allows us to improve the precision of our near- to mid-infrared color sequences.
The WFC3 grism observations are slitless and therefore roll angle constraints must be placed on the observations in order to avoid contamination of the target by other sources in the field. In our previous Cycle 18 and 19 programs (#12330 and #12544, 16 orbits in total) we attempted to derive roll angles using ground-based observations but unfortunately several of the spectra in the Cycle 18 program were still contaminated by nearby stars. In order to eliminate any possibility of contamination, we will first observe each candidate through the F125W filter alone so that we can use the resulting images and aXeSIM to derive precise, contamination-free roll angles which will then be entered in to the APT.
Due to various constraints, not all of the eighteen targets listed in Table 1 will be observed in all three modes. Four of the targets are in our Cycle 18 and 19 programs to obtain G141 grism observations (WISE 0535, WISE 1405, WISE 1828, and WISE 2209) and therefore do not require F125W imaging. The G141 spectrum of the first Y dwarf WISE 1828 did not have sucient S/N (<4 at the peak of the J-band) so we will re-observe it in this program. Twelve of the candidates fall within Cycle 20's unrestricted RA zones and can be scheduled for G102/G141 spectroscopic observations once their roll angle restrictions are calculated. The other three will have to wait until Cycle 21 for spectroscopy at which time we will submit a second proposal. We prefer to obtain the F125W images of these objects now, however, as the time baseline between this observation and the images in Cycle 21 will help with our ancillary, astrometric science, described in S4. In addition, we will be able to include roll angle constraints at the time of submission to expedite the observations and increase scheduling flexibility.
Based on our previous experience with the spectral classification and modeling of late- type T and Y dwarf spectra, we require a minimum S/N of 10/20 at the peaks of the Y /J bands and a S/N of 30 for the direct images. We used the spectrum of the T9 dwarf UGPS 0722-05 (absolutely flux calibrated to the observed J-band magnitudes of each target) and the WFC3 Exposure Time Calculator to estimate the exposure time needed to reach the required S/N. Note that for the faintest sources, we reduced the S/N requirement slightly in order to obtain the data in a reasonable number of orbits. The number of orbits required for each object (including all overheads) is given in columns 7-9 of Table 1. In total, we request 125 orbits to complete this program.
The schedulability of this program is clearly of concern given the large number of orbits requested. However the fourteen orbits of F125W imaging have no constraints, although we request that they be scheduled as soon as possible so that we can derive the roll angle constraints for the grism observations. The grism observations require roll angle constraints to avoid contamination but they typically do not limit the observability of the targets dra- matically as can be seen by inspecting the Visit Planner for WISE 1828 and WISE 1405.
COOL STARS
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SUPPORTED
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BROWN DWARF
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J2000
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STAR
BROWN DWARF
J2000
J2000
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STAR
BROWN DWARF
J2000
J2000
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STAR
BROWN DWARF
J2000
J2000
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STAR
BROWN DWARF
J2000
J2000
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STAR
BROWN DWARF
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STAR
BROWN DWARF
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STAR
BROWN DWARF
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STAR
BROWN DWARF
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BROWN DWARF
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STAR
BROWN DWARF
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STAR
BROWN DWARF
J2000
J2000
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STAR
BROWN DWARF
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STAR
BROWN DWARF
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STAR
BROWN DWARF
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BROWN DWARF
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BROWN DWARF
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WFC3/IR
Imaging
No
No
F125W
WFC3/IR
Imaging
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No
F125W
WFC3/IR
Imaging
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No
F125W
WFC3/IR
Imaging
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No
F125W
WFC3/IR
Imaging
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No
F125W
WFC3/IR
Imaging
No
No
F125W
WFC3/IR
Imaging
No
No
F125W
WFC3/IR
Imaging
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No
F125W
WFC3/IR
Imaging
No
No
F125W
WFC3/IR
Imaging
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No
F125W
WFC3/IR
Imaging
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No
F125W
WFC3/IR
Imaging
No
No
F125W
WFC3/IR
Imaging
No
No
F125W
WFC3/IR
Imaging
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No
F125W
WFC3/IR
Imaging
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No
F098M
WFC3/IR
Spectroscopic
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No
G102
WFC3/IR
Imaging
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No
F125W
WFC3/IR
Spectroscopic
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No
G141
WFC3/IR
Imaging
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No
F098M
WFC3/IR
Spectroscopic
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No
G102
WFC3/IR
Imaging
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No
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Spectroscopic
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No
G141
WFC3/IR
Imaging
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F098M
WFC3/IR
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WFC3/IR
Imaging
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No
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No
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WFC3/IR
Imaging
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No
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WFC3/IR
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WFC3/IR
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No
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WFC3/IR
Imaging
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WFC3/IR
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No
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No
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No
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WFC3/IR
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No
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No
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No
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No
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WFC3/IR
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No
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WFC3/IR
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No
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WFC3/IR
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No
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WFC3/IR
Imaging
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No
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WFC3/IR
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No
G102
WFC3/IR
Imaging
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No
F125W
WFC3/IR
Spectroscopic
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G141
POS-TARG
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