0
Assigned ID: 440
----- Attempting Submission 1 (Fri Apr 07 08:30:42 GMT 2017) -----
HST Phase I Proposal 440 (lris_z3lyc_cycle25.apt) successfully submitted.
Receipt: # 440-1
----- Attempting Submission 2 (Fri Apr 07 18:21:02 GMT 2017) -----
HST Phase I Proposal 440 (lris_z3lyc_cycle25.apt) successfully submitted.
Receipt: # 440-2
----- Attempting Submission 3 (Fri Apr 07 19:39:38 GMT 2017) -----
HST Phase I Proposal 440 (lris_z3lyc_cycle25.apt) successfully submitted.
Receipt: # 440-3
----- Attempting Submission 4 (Fri Apr 07 19:53:09 GMT 2017) -----
HST Phase I Proposal 440 (lris_z3lyc_cycle25.apt) successfully submitted.
Receipt: # 440-4
We have added Group <visits> within <time> constraints, to ensure that the F606W, F125W, F160W datasets are taken close together for each target.
9/14/17 - Royle - Expanded GROUP WITHIN to 90 days for visits 10-14 due to guide star availability
11/05/18 - ROYLE - Updates to target #17 to open up windows for visits 17 and 18, made on behalf of PI
11/06/18 - ROYLE - Added ORIENT to visit 17 to exclude U3 51-63 as requested by PI
-185705828
----- Attempting Submission 1 (Fri Jul 14 21:22:01 GMT 2017) -----
----- Attempting Submission 2 (Tue Jul 18 22:51:28 GMT 2017) -----
----- Attempting Submission 3 (Fri Sep 08 19:04:03 GMT 2017) -----
----- Attempting Submission 4 (Thu Sep 14 17:29:24 GMT 2017) -----
----- Attempting Submission 5 (Mon Nov 05 22:04:09 GMT 2018) -----
----- Attempting Submission 7 (Tue Nov 06 19:25:22 GMT 2018) -----
in-house processing
The Path Forward for Lyman-Continuum Studies at z~3
Escaping Lyman-continuum (LyC) radiation from star-forming galaxies is likely responsible for the reionization of the universe. However, the direct measurement of escaping LyC radiation has proven exceptionally challenging, with only a few robust LyC detections at z~3, the highest redshift at which such measurements are possible. The tiny sample size of confirmed LyC sources hinders efforts to estimate the average LyC escape fraction and trace how its value depends on other galaxy properties -- both crucial for estimating the contribution of galaxies to reionization at z>6. To understand the LyC properties of distant galaxies, we must assemble a significantly larger sample of candidate LyC leakers and subject them to rigorous vetting for foreground contamination. Based on deep Keck/LRIS spectroscopy of 124 z~3 star-forming galaxies, we have identified 15 galaxies with apparent detections of LyC radiation. We now require HST imaging to remove any low-redshift contamination on an object-by-object basis, connect the ionizing and non-ionizing properties of LyC leakers, and compare the spatially-resolved stellar populations and morphologies of LyC detections and non-detections. We propose for 87 orbits of deep ACS/F606W, WFC3/F125W and WFC3/160W observations, providing multi-band coverage for the 14 LyC detections lacking HST data, as well as a control sample of 26 galaxies with deep Keck/LRIS spectra and LyC non-detections, and 37 additional galaxies spectroscopically confirmed at z~3. Analysis of these data will robustly remove low-redshift contaminants, revealing the connection between LyC leakage and galaxy properties both at z~3 and during the epoch of reionization.
Pointings and Sample:
We propose deep ACS/F606W (V), WFC3/IR/F125W (J), and WFC3/IR/F160W (H) imaging in targeted pointings across five different Lyman Break Galaxy (LBG) survey fields. Our observations total 11 WRC3/IR pointings with coverage in both F125W and F160W, and 7 ACS pointings with coverage in F606W. Our highest priority targets are a sample of 14 LBGs with apparent spectroscopic Lyman-continuum (LyC) detections. Our primary goals are (1) to estimate robust photometric redshifts for all morphological subcomponents associated with these LyC detections, and therefore obtain a clean sample of high-redshift LyC detections with detailed stellar population and morphological information. Deep multi-band imaging with the proposed filter set will result in robust photometric redshifts, and the removal of low-redshift contaminants; (2) to determine spatially-resolved stellar populations of LyC emitters; (3) to measure the morphologies of LyC emitters; and (4) to connect f_esc, the escape fraction of LyC emission, with other galaxy properties. Furthermore, with a large set of spectroscopic LyC non-detections at z~3 imaged by HST within the same pointings, we will conduct a differential comparison between the spatially-resolved stellar populations and morphologies of objects with and without leaking LyC emission.
ORIENT strategy:
As our z~3 targets are distributed across each pointing, the allowed range of ORIENT angles that enables the maximum number of targets is
fairly constrained in some cases. For each visit with ORIENT constraints, we specify the range of allowed ORIENT angles, which optimizes the number of targets covered.
Orbit / visit strategy:
Each F606W, F125W, and F160W pointing is executed in a 3-orbit visit, broken down into 3 single-orbit, 4-exposure dither patterns. The proposed program requires 87 orbits (7x3 orbits in F606W, 11x3 orbits in F125W, and 11x3 orbits in F160W).
Dither Strategy:
The 12 exposures for each F606W visit are executed as a set of 3, 4-point ACS-WFC-DITHER-BOX patterns. The 12 exposures for each WFC3/IR orbit (F125W and F160W) are executed as a set of 3, 4-point WFC3-IR-DITHER-LINE patterns. For WFC3/IR observations, we apply
POS-TARG offsets between each dither pattern to improve the PSF sampling, and reduce the effects of bad pixels and droplets.
Galaxies and the IGM
0
false
false
false
false
false
false
false
SUPPORTED
GALAXY
HIGH REDSHIFT GALAXY
J2000
J2000
GALAXY
HIGH REDSHIFT GALAXY
J2000
J2000
GALAXY
HIGH REDSHIFT GALAXY
J2000
J2000
GALAXY
HIGH REDSHIFT GALAXY
J2000
J2000
GALAXY
HIGH REDSHIFT GALAXY
J2000
J2000
GALAXY
HIGH REDSHIFT GALAXY
J2000
J2000
GALAXY
HIGH REDSHIFT GALAXY
J2000
J2000
GALAXY
HIGH REDSHIFT GALAXY
J2000
J2000
GALAXY
HIGH REDSHIFT GALAXY
J2000
J2000
GALAXY
HIGH REDSHIFT GALAXY
J2000
J2000
GALAXY
HIGH REDSHIFT GALAXY
J2000
J2000
GALAXY
HIGH REDSHIFT GALAXY
J2000
J2000
GALAXY
HIGH REDSHIFT GALAXY
J2000
J2000
GALAXY
HIGH REDSHIFT GALAXY
J2000
J2000
GALAXY
HIGH REDSHIFT GALAXY
J2000
J2000
GALAXY
HIGH REDSHIFT GALAXY
J2000
J2000
GALAXY
HIGH REDSHIFT GALAXY
J2000
J2000
GALAXY
HIGH REDSHIFT GALAXY
J2000
J2000
WFC3/IR
Imaging
No
No
F125W
WFC3/IR
Imaging
No
No
F160W
ACS/WFC
Imaging
No
No
F606W
WFC3/IR
Imaging
No
No
F125W
WFC3/IR
Imaging
No
No
F160W
ACS/WFC
Imaging
No
No
F606W
WFC3/IR
Imaging
No
No
F125W
WFC3/IR
Imaging
No
No
F160W
WFC3/IR
Imaging
No
No
F125W
WFC3/IR
Imaging
No
No
F160W
ACS/WFC
Imaging
No
No
F606W
WFC3/IR
Imaging
No
No
F125W
WFC3/IR
Imaging
No
No
F160W
ACS/WFC
Imaging
No
No
F606W
WFC3/IR
Imaging
No
No
F125W
WFC3/IR
Imaging
No
No
F160W
ACS/WFC
Imaging
No
No
F606W
WFC3/IR
Imaging
No
No
F125W
WFC3/IR
Imaging
No
No
F160W
WFC3/IR
Imaging
No
No
F125W
WFC3/IR
Imaging
No
No
F160W
ACS/WFC
Imaging
No
No
F606W
WFC3/IR
Imaging
No
No
F125W
WFC3/IR
Imaging
No
No
F160W
WFC3/IR
Imaging
No
No
F125W
WFC3/IR
Imaging
No
No
F160W
WFC3/IR
Imaging
No
No
F125W
WFC3/IR
Imaging
No
No
F160W
ACS/WFC
Imaging
No
No
F606W
POS-TARG
DITHER
0.262
LINE
0.192
false
false
68.14
4
18.39
ACS-WFC-DITHER-BOX
2
false
POS-TARG
DITHER
0.636
LINE
false
false
4
41.788
WFC3-IR-DITHER-LINE
3
false
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