0
Assigned ID: 359
----- Attempting Submission 1 (Fri Apr 10 04:41:56 GMT 2015) -----
HST Phase I Proposal 359 (lya_grism_submit.pdf.apt.2015_04_07_21_54.aptbackup) successfully submitted.
Receipt: # 359-1
----- Attempting Submission 2 (Fri Apr 10 20:45:04 GMT 2015) -----
HST Phase I Proposal 359 (lya_grism_submit.pdf.apt.2015_04_07_21_54.aptbackup) successfully submitted.
Receipt: # 359-2
----- Attempting Submission 3 (Fri Apr 10 21:41:08 GMT 2015) -----
HST Phase I Proposal 359 (lya_grism_submit.pdf.apt.2015_04_07_21_54.aptbackup) successfully submitted.
Receipt: # 359-3
Updated visits 46, 56, and 61 to put the F105W direct imaging
at the end of each orbit (and the G102 grism observatons at the beginning of each orbit.
856530131
----- Attempting Submission 1 (Thu Jul 23 05:13:20 GMT 2015) -----
HST Phase II Proposal 14227 (lya_grism_submit.pdf.apt.2015_04_07_21_54.aptbackup) successfully submitted.
Receipt: # 14227-1
----- Attempting Submission 2 (Thu Jul 23 05:15:54 GMT 2015) -----
HST Phase II Proposal 14227 (lya_grism_submit.pdf.apt.2015_04_07_21_54.aptbackup) successfully submitted.
Receipt: # 14227-2
----- Attempting Submission 3 (Thu Jul 23 19:20:20 GMT 2015) -----
----- Attempting Submission 4 (Mon Sep 21 21:27:28 GMT 2015) -----
----- Attempting Submission 5 (Tue Sep 22 14:58:26 GMT 2015) -----
----- Attempting Submission 6 (Sat Oct 03 13:32:17 GMT 2015) -----
----- Attempting Submission 7 (Wed Oct 07 17:35:29 GMT 2015) -----
----- Attempting Submission 8 (Sat Oct 10 13:42:39 GMT 2015) -----
----- Attempting Submission 9 (Tue Jan 19 16:24:10 GMT 2016) -----
----- Attempting Submission 10 (Fri Jan 22 14:45:59 GMT 2016) -----
----- Attempting Submission 11 (Sat Feb 06 13:30:26 GMT 2016) -----
----- Attempting Submission 12 (Wed Mar 02 19:39:31 GMT 2016) -----
----- Attempting Submission 13 (Tue Mar 08 14:22:20 GMT 2016) -----
----- Attempting Submission 14 (Tue May 03 16:43:24 GMT 2016) -----
----- Attempting Submission 15 (Thu Jul 14 18:27:33 GMT 2016) -----
Your proposal could not be saved.
Submission aborted.
----- Attempting Submission 16 (Mon Sep 12 22:13:29 GMT 2016) -----
I reran the Visit Planner for Visits 46, 56. and 61, which produced no errors. (These are the only visits I changed).
The CANDELS Lyman-alpha Emission At Reionization (CLEAR) Experiment
One of the most promising probes of reionization is the evolution of Ly-alpha emission from galaxies at z>6.5. We propose to measure the evolution of the strength of Ly-alpha emission in galaxies at z=6.5-8.2 using 16 pointings to 12 orbit depth with the WFC3/G102 grism in the deep CANDELS fields (including 4 pointings with existing data). The data will be sensitive to low line fluxes, and rest-frame Ly-alpha equivalent widths as low as 40-60 Angstroms for galaxies at H(AB)=27 mag. By targeting in CANDELS, our objects have the highest quality dataset of any fields on the sky, which provides high-redshift galaxy samples with the highest fidelity and enables the efficient rejection of contaminants. A clear advantage of the G102 grism over ground-based telescopes is that it provides stable image quality and a smooth sensitivity function over the wavelength range, 0.85-1.15 micron (without terrestrial effects of night sky lines), covering Ly-alpha from all galaxies with z=6 to 8.2. Our survey will provide spectroscopic observations of Ly-alpha in 90 (105) star-forming galaxies with z=7-8.2 (6.5-7.0), making it the largest, deepest, homogeneous survey of its kind and quadrupling the area in CANDELS covered with deep G102 spectroscopy. Our proposal goals are: 1. Provide spectroscopic redshifts for hundreds of z=1-8 galaxies fainter than ground based limits (including 90 at z>7); 2. Provide the most robust measurement yet of the Ly-alpha detection fraction and its evolution for galaxies at these redshifts; 3. Measure the evolution of the Ly-alpha distribution function and discern between models of the evolution of Ly-alpha emission.
Observing Description for HST Cycle 23 Proposal 14227
PI: Casey Papovich (papovich@physics.tamu.edu)
We will observe 12 fields with deep (12 orbit-depth) WFC3/G102
spectroscopy. The fields are divided into two areas on the sky:
- 6 fields in the CANDELS GOODS-S field (3h32m, -27d)
- 5 of the fields (GS2, GS1, GS5, GS4, GS3) will receive 12
orbits, divided in 6 visits of 2 orbits per visit.
- 1 field (the ERS) already has 2 orbit G102 depth from. We
will observe 10 more orbits, divided into 5 visits of 2 orbits
per visit.
- 6 fields in the CANDELS GOODS-N field (12h36m, +62d)
- all 6 fields have existing 2-orbit G102 coverage. We will
observe each field with 10 more orbits, divided into 5 visits
of 2 orbits per visit.
EXPOSURES/VISITS: Each visit will consist of 2 orbits. Each orbit
will include 1 direct image and 2 longer grism observations.
ORIENTS: It is our intent that each visit of each field have a unique ORIENT.
We have not yet constrained the ORIENT in the phase II. We would like
each visit to be more-or-less random in ORIENT, but we require that
each subsequent visit have an ORIENT at least +/- 8 deg from the other
ORIENTS for each field. (The point is to never have two ORIENTs close
to each other, because the different ORIENTs are to guard against
contamination and detector defects). We would welcome input from the
program coordinator about how to configure the observations to ensure
good ORIENT spacing for each visit of each target.
Two of pointings (GN1 and GS1) are near the edge of the field where we
have the deep HST imaging. We will want to have the ORIENT there such
that spectra from "contaminants" (whose direct imaging falls off the
chip but their spectra are thrown onto the chip) can be identified in
the images. In both cases, we will want to use ORIENTS that constrain.
DITHERS: There are 4 grism exposures per visit, and each is to have a
different dither position (the direct images will have the same dither
position as the 1st grism exposure of each orbit). We have copied
the dither positions from the 3DHST survey, where we also move the
first dither position with an offset in the X-direction by about -14"
pixels to ensure that the 1st order grism spectra fall on the chip
given the selected field center. The initial position in the
Y-direction is -5.077" to place the center of the GRISM1024 aperture
close to the center of rotation,maximizing the overlap of the
different visits regardless of ORIENT. The dither offsets are
designed to move in a box of 1/2-integer pixel shifts.
SCHEDULING: Our targets are the faint emission lines from very
distant galaxies. As such, we need the lowest possible backgrounds for
our grism exposures. We want to sequencing the exposures in each
orbit to minimize the effect of intra-orbit varying background (e.g.,
from the HeI 1.08 micron emission in the Earth's upper atmosphere;
Brammer et al. ISR WFC3 2014-03). Before each HST visit, we would
like our STScI Co-Investigators (G. Brammer, J. Lotz) to work with the
contact scientist and program coordinator to adjust the sequence of
exposures in an orbit depending on when the observations are scheduled
relative to the expected limb angle and Earth shadowing. This will
only require that we possibly swing the sequencing of the direct
imaging and grism exposures so that the direct imaging occurs during
periods of higher IR background, and the grism exposures occurs during
the periods of lower IR background in each orbit. This approach was
very successful for the HST Frontier Fields in mitigating the impact
of high and variable IR sky on F105W exposures, and resulted in a
significant increase in the effective depth of the data.
------------------------------------------------------------
COSMOLOGY
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UNIDENTIFIED
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UNIDENTIFIED
BLANK FIELD
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WFC3/IR
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G102
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G102
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No
G102
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No
G102
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G102
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No
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No
No
G102
WFC3/IR
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No
No
G102
WFC3/IR
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No
No
G102
WFC3/IR
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