0
Assigned ID: 3988
----- Attempting Submission 1 (Sat May 20 19:55:16 GMT 2023) -----
HST Phase I Proposal 3988 successfully submitted.
Receipt: # 3988-1
----- Attempting Submission 2 (Wed May 24 16:29:38 GMT 2023) -----
HST Phase I Proposal 3988 successfully submitted.
Receipt: # 3988-2
----- Attempting Submission 3 (Wed May 24 22:47:16 GMT 2023) -----
0
----- Attempting Submission 1 (Wed Sep 13 18:42:41 GMT 2023) -----
----- Attempting Submission 2 (Tue Oct 10 10:04:59 GMT 2023) -----
----- Attempting Submission 3 (Thu Oct 12 20:52:20 GMT 2023) -----
----- Attempting Submission 4 (Mon Dec 04 22:09:39 GMT 2023) -----
Your proposal could not be saved.
Submission aborted.
----- Attempting Submission 5 (Thu Dec 07 11:03:24 GMT 2023) -----
----- Attempting Submission 6 (Thu Feb 01 17:02:03 GMT 2024) -----
The following items have been discussed with the PC, and are no issues.
A Fundamental Test of Black Hole Masses: Ultraviolet Echo Mapping the Multi-Scale Broad Line Gas around Quasars
We propose a novel spectroscopic ultraviolet monitoring campaign that uses the STIS/MAMA G230L grating to map the broad-line gas and assess its role as a mass estimator across a wide range of ionization conditions in two luminous quasars. Recent studies of a more diverse sample of AGN have unveiled shortcomings in the fundamental framework for black-hole mass measurements. This experiment presents a new test of the reliability of black-hole mass measurements over cosmic time in two sources that are selected to be representative of a previously unexplored region of the broader AGN population, with higher luminosity, accretion rate, and significantly shorter optical Hb lag compared to the existing AGN samples. Previous RM measurements of stratified UV/optical broad-line regions exist for only six well-studied, local, low-luminosity AGN. We propose to use HST/STIS to monitor the strong UV broad emission lines (Lya and CIV), supported by contemporaneous spectroscopic monitoring from SDSS-V for the lower ionization and more distant optical broad emission lines. We analyze comprehensive light curve simulations using the proposed 3-day cadence, 75-day duration, and 1-orbit depth per epoch to demonstrate that our observations will successfully measure broad-line region sizes, map emission-line gas, and test the reliability of black-hole mass estimators for two luminous quasars that are representative of the bulk of black hole mass assembly over cosmic time.
Observing Description Proposal 17487
The goal of this proposal is to obtain ultraviolet (UV) monitoring of the broad line region (BLR) of two luminous quasars that are selected to be representative of the broader AGN population, and obtain the reverberation mapping time delay (lag) of high-ionization, UV emission lines that are closer to the central source and compare with low-ionization, optical emission lines that are more distant from the central source. The wide range of ionization conditions covered by UV monitoring of strong BLR emission lines and connecting it to the optical lines can assess their role as a black hole mass estimator over cosmic time.
Coordinated monitoring: Groundbased spectroscopy and photometry:
Given that our primary science goal is to simultaneously monitor high-ionization, UV emission lines using HST and the low ionization emission lines using contemporaneous ground-based spectroscopic monitoring from SDSS-V, it is critically important that the HST observations occur during the January - June window when these quasars are observed with SDSS-V. Furthermore, to measure the reverberation time delay (lag), we need coordinated ground-based photometry to map the optical continuum bands (using LCOGT and Liverpool Telescope). While these targets are observable from the ground during the January - June window, we also need ground-based photometry to begin a few weeks ahead of the HST observations to track the continuum variation before the beginning of the HST observation. Therefore, the most suitable window for observing these targets is from February 1 until mid-June. However, an earlier start of the program between mid-January to mid-June could also be viable.
Program Cadence and Duration:
We request a 75-day duration for our program, where 25 orbits are dedicated to each target using an approximately 3-day cadence, totaling 50 orbits. We use the 11-year observed optical continuum and 7-year spectroscopic light curves from the SDSS-RM observations (Shen et al. 2023) to ensure the lag detection succeeds with the requested cadence and duration. Ideally, the observations should be made three days apart, although this can be relaxed to accommodate target visibility or time-critical observations. We emphasize that evenly spaced intervals are not required so long as the average of 3 days is maintained over the duration of the program. Based on the record of previous reverberation campaigns in Cycle 25 and 26, we expect a 3-day cadence with a jitter of +/- 0.5 days to have marginal effects on detecting a reliable lag.
Impact of Data Losses:
During this program's duration, data losses due to instrument or spacecraft safing events or guide-star acquisition failure may occur. We expect that approximately 1-2 gaps that result in 5-6 days losses each have a limited effect on our lag detectibility. Also, noisy gyros have led to an increase in guide star acquisition failures. We expect a current failure of 10%. However, suppose guide-star acquisition failures are more than 10% in the early stages of the program. In that case, we ask to add additional visits to the nominal end of the program to replace the unsuccessful visits.
Our team has extensive experience with quasars, reverberation mapping, the R-L relation, and HST monitoring with STIS. Most of the proposal team are members of the SDSS Reverberation Mapping project. Co-I Brandt is the PI of the SDSS-RM campaign, and Co-I Shen is the PI of SDSS-RM and SDSS-V Black Hole Mapper survey.
PI Homayouni has experience in designing, reducing, and publishing HST UV monitoring programs and will coordinate the team's work and lead the analysis and interpretation of the data.
Co-I Trump is the SDSS-V Black Hole Mapper Targetting and Cadence Coordinator and will supervise the SDSS-V Black Hole Mapper RM design developed by Co-I Davis. We have full access to the SDSS-RM and SDSS-V data, both preceding and during the proposed HST monitoring. Co-Is Trump and Davis will also participate in analyzing and interpreting the data.
Co-Is Kriss, De Rosa, and Koekemoer are HST instrument experts and will aid in the STIS data reduction and analysis.
Co-Is Schneider, Grier, Li, Mehdipour, and Sturm have experience designing and reducing spectra and HST imaging and will assist in the interpretation of the data.
Co-Is Fonseca Alvarez and Sharp have experience designing and reducing LCO observations and have developed all necessary software for coordinated ground-based optical monitoring.
Co-I Horne and Fries are experts on emission line reverberation mapping. Through co-I Horne, we also have access to coordinated queue-mode optical monitoring to match the HST UV observations: institutional access to the Liverpool Telescope and allocated Key Project time on the LCOGT network.
Co-Is Hall, Kriss, and Mehdipour are experts in studying quasar properties and outflows and will contribute to the data analysis and interpretation.
Co-I Cackett is an expert in continuum reverberation mapping. Through Co-I Cackett, we also have institutional access to Zowada Observatory, which provides supplementary photometry for our target.
Co-I Assef is an expert in studies of properties of luminous quasars and will contribute to the interpretation of the data.
Co-I Ho and Kakkad are experts in studies of high-redshift AGN and scaling relations and will assist in the implications of the observations for quasar populations.
Co-I Temple is an emission line and photoionization modeling expert and will assist in interpreting the geometry and structure of ionized gas.
We anticipate supplementing this with additional LCOGT time through NOAO: several similar LCO proposals in previous years have been successful.
Supermassive Black Holes and Active Galaxies
6
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No
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G230L
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Imaging
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No
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