0
Assigned ID: 797
----- Attempting Submission 1 (Fri Apr 10 20:44:15 GMT 2015) -----
0
----- Attempting Submission 1 (Thu Jul 16 15:19:39 GMT 2015) -----
Are High-Redshift Spectroscopic Black Hole Mass Estimates Biased?
Black hole (BH) masses estimated from single-epoch spectroscopy
underlie our understanding of the build-up of BHs from high redshift
to the present, but are currently based on a small sample of low-L,
low-z "reverberation mapped" (RM) AGNs. The existing sample of RM
AGNs appears to be biased against quasars where a radiation line
driven disk-wind dominates the broad emission line region (BELR). As
such, we propose UV spectroscopy of 25 SDSS quasars at z~0.5 that have
luminosities comparable to the existing RM quasars, but that are more
representative of the BELR properties of the average quasar. These
data will enable us to confirm the bias in the RM quasar sample and
lay the groundwork for reverberation mapping of quasars where winds
affect the BELR. This work is important because successful RM
measurements of local AGNs have not been extended to the high-z,
high-L regime, requiring extrapolation methods from low redshift. The
best tool for this work comes from UV observations of the CIV emission
line region where it is possible to distinguish between virial- and
wind-dominated BELRs. These measurements will further enable us to
inter-compare BH masses computed using measurements from CIV, MgII,
and Hbeta for each quasar. For this work we require spectral coverage
of all the optical and UV broad emission lines (Ly-apha to H-beta) to
characterize the diversity of quasar spectra, which we will then
relate to BH mass, accretion rate and accretion disk physics. These
data will provide a powerful UV legacy database for investigations of
the BELR structures of all quasars in addition to more robust
bootstrapping of BH mass estimates from low to high redshift.
Each quasar will be observed with STIS/CCD and G230LB grating which covers 1680<lambda <3060 (observed; 1120<lambda <2040 at z~0.5) using the 52"x0.2" slit at position E1. CCD observations are preferred over MAMA observations since we do not require time resolution and the CCD as better throughput at lambda>2400 Angstroms. STIS is preferred over COS because of the desire to cover not just CIV at 1550 Angstroms, but all of the UV lines between Ly-alpha (1216 Ang) and CIII] (1909 Ang) which STIS can do at one time, but COS needs multiple grating tilts for. However, the observations could be done with COS if it became necessary (with lower S/N at CIII]).
Targets were selected from the SDSS and matched to GALEX catalogs in order to obtain UV fluxes to estimate HST exposure times. One orbit (>=54 minutes) is enough for each of our observations. We allow for 18 minutes of overhead for each object, which includes 6 minutes for guide star acquisition, 6 minutes for target acquisition, 5 minutes for CCD overhead and 1 minute for CR-splitting. Target acquisition exposure times (with STIS/CCD) were calculated to achieve S/N > 40 over a 3x3 pixel checkbox, based on their SDSS optical magnitudes. No "peak-up" should be needed for the 0.2" slit. The remaining 2160 seconds allows us to achieve a S/N of 7 in the continuum at rest-frame 1550 Angstroms for the faintest quasar in our sample. Moderate S/N is needed because we are trying to measure accurate line profiles and precise redshifts, in contrast to the accuracy of the redshift that one gets from a S/N~3 spectrum. Our expected S/N also means that individual CR-split exposures will not be read-noise limited.
AGN/QUASARS
0
false
true
false
false
false
0.0
0.0
false
SUPPORTED
GALAXY
QSO
J2000
J2000
NUV = 18.12, g=17.62
GALAXY
QSO
COS coverage of Ly-alpha emission, but not the CIV emission line, so not a duplicate.
J2000
J2000
NUV = 17.92, g=17.37
GALAXY
QSO
J2000
J2000
NUV = 18.35, g=17.62
GALAXY
QSO
J2000
J2000
NUV = 18.15, g=17.45
GALAXY
QSO
J2000
J2000
NUV = 18.48, g=17.49
GALAXY
QSO
Recent COS coverage of the Ly-alpha emission line, but not of the CIV emission line, so no duplicate.
J2000
J2000
NUV = 17.85, g=17.51
GALAXY
QSO
J2000
J2000
NUV = 17.80, g=17.56
GALAXY
QSO
J2000
J2000
NUV = 16.10, g=15.7
GALAXY
QSO
J2000
J2000
NUV = 18.32, g=17.71
GALAXY
QSO
J2000
J2000
NUV = 18.30, g=17.56
GALAXY
QSO
J2000
J2000
NUV = 18.06, g=17.51
GALAXY
QSO
J2000
J2000
NUV = 17.99, g=17.51
GALAXY
QSO
Existing COS coverage of the Ly-alpha forest, but not the CIV emission line, so not a duplicate.
J2000
J2000
NUV = 18.29, g=17.66
GALAXY
QSO
J2000
J2000
NUV = 17.89, g=17.51
GALAXY
QSO
Existing COS coverage of the Ly-alpha forest, but not the CIV emission line, so not a duplicate.
J2000
J2000
NUV = 18.11, g=17.52
GALAXY
QSO
J2000
J2000
NUV = 18.43, g=17.17
GALAXY
QSO
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NUV = 17.55, g=17.39
GALAXY
QSO
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GALAXY
QSO
J2000
J2000
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GALAXY
QSO
J2000
J2000
NUV = 17.84, g=17.35
GALAXY
QSO
J2000
J2000
NUV = 18.18, g=17.28
GALAXY
QSO
J2000
J2000
NUV = 17.98, g=17.37
GALAXY
QSO
J2000
J2000
NUV = 18.10, g=17.57
GALAXY
QSO
J2000
J2000
NUV = 18.25, g=17.62
GALAXY
QSO
J2000
J2000
NUV = 17.89, g=17.43
STIS/CCD
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No
G230LB
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No
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No
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Spectroscopic
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No
G230LB
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STIS/CCD
Spectroscopic
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No
G230LB
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STIS/CCD
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