Accretion Disk Size and Updated Time-delay Measurements in the Gravitationally Lensed Quasar SDSS J165043.44+425149.3

We analyze variability in 15-season optical lightcurves from the doubly imaged lensed quasar SDSS J165043.44+425149.3 (SDSS1650), comprising five seasons of monitoring data from the Maidanak Observatory (277 nights in total, including the two seasons of data previously presented in Vuissoz et al.),...

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Main Authors: A. B. Rivera, C. W. Morgan, S. M. Florence, K. Kniezewski, M. Millon, F. Courbin, S. E. Dahm, F. J. Vrba, T. M. Tilleman, M. A. Cornachione, I. M. Asfandiyarov, S. A. Ehgamberdiev, O. A. Burkhonov
Format: Article
Language:English
Published: IOP Publishing 2024-01-01
Series:The Astrophysical Journal
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Online Access:https://doi.org/10.3847/1538-4357/ad3069
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author A. B. Rivera
C. W. Morgan
S. M. Florence
K. Kniezewski
M. Millon
F. Courbin
S. E. Dahm
F. J. Vrba
T. M. Tilleman
M. A. Cornachione
I. M. Asfandiyarov
S. A. Ehgamberdiev
O. A. Burkhonov
author_facet A. B. Rivera
C. W. Morgan
S. M. Florence
K. Kniezewski
M. Millon
F. Courbin
S. E. Dahm
F. J. Vrba
T. M. Tilleman
M. A. Cornachione
I. M. Asfandiyarov
S. A. Ehgamberdiev
O. A. Burkhonov
author_sort A. B. Rivera
collection DOAJ
description We analyze variability in 15-season optical lightcurves from the doubly imaged lensed quasar SDSS J165043.44+425149.3 (SDSS1650), comprising five seasons of monitoring data from the Maidanak Observatory (277 nights in total, including the two seasons of data previously presented in Vuissoz et al.), five seasons of overlapping data from the Mercator telescope (269 nights), and 12 seasons of monitoring data from the US Naval Observatory, Flagstaff Station at lower cadence (80 nights). We update the 2007 time-delay measurement for SDSS1650 with these new data, finding a time delay of ${\rm{\Delta }}{t}_{\mathrm{AB}}=-{55.1}_{-3.7}^{+4.0}$ days, with image A leading image B. We analyze the microlensing variability in these lightcurves using a Bayesian Monte Carlo technique to yield measurements of the size of the accretion disk at λ _rest = 2420 Å, finding a half-light radius of log( r _1/2 /cm) = ${16.19}_{-0.58}^{+0.38}$ assuming a 60° inclination angle. This result is unchanged if we model 30% flux contamination from the broad-line region. We use the width of the Mg ii line in the existing Sloan Digital Sky Survey spectra to estimate the mass of this system’s supermassive black hole, finding M _BH = 2.47 × 10 ^9 M _⊙ . We confirm that the accretion disk size in this system, whose black hole mass is on the very high end of the M _BH scale, is fully consistent with the existing quasar accretion disk size–black hole mass relation.
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spelling doaj.art-ae7d8d01c2b745a38350ef5ff827c07f2024-03-29T15:26:28ZengIOP PublishingThe Astrophysical Journal1538-43572024-01-01964217310.3847/1538-4357/ad3069Accretion Disk Size and Updated Time-delay Measurements in the Gravitationally Lensed Quasar SDSS J165043.44+425149.3A. B. Rivera0https://orcid.org/0000-0001-8125-1669C. W. Morgan1https://orcid.org/0000-0003-2460-9999S. M. Florence2K. Kniezewski3M. Millon4https://orcid.org/0000-0001-7051-497XF. Courbin5https://orcid.org/0000-0003-0758-6510S. E. Dahm6https://orcid.org/0000-0002-2968-2418F. J. Vrba7T. M. Tilleman8M. A. Cornachione9https://orcid.org/0000-0003-1012-4771I. M. Asfandiyarov10S. A. Ehgamberdiev11O. A. Burkhonov12Department of Physics, United States Naval Academy , 572C Holloway Road, Annapolis, MD 21402, USA ; cmorgan@usna.edu; University of Pennsylvania Libraries , 3420 Walnut Street, Philadelphia, PA 19104, USADepartment of Physics, United States Naval Academy , 572C Holloway Road, Annapolis, MD 21402, USA ; cmorgan@usna.eduDepartment of Physics, United States Naval Academy , 572C Holloway Road, Annapolis, MD 21402, USA ; cmorgan@usna.eduDepartment of Physics, United States Naval Academy , 572C Holloway Road, Annapolis, MD 21402, USA ; cmorgan@usna.eduKavli Institute for Particle Astrophysics and Cosmology, Stanford University , Stanford, CA 94305, USAInstitute of Physics , Laboratory of Astrophysics, Ecole, Polytechnique Fédérale de Lausanne (EPFL), Observatoire de Sauverny, 1290 Versoix, SwitzerlandUnited States Naval Observatory , Flagstaff Station, 10391 West Naval Observatory Road, Flagstaff, AZ 86005, USAUnited States Naval Observatory , Flagstaff Station, 10391 West Naval Observatory Road, Flagstaff, AZ 86005, USAUnited States Naval Observatory , Flagstaff Station, 10391 West Naval Observatory Road, Flagstaff, AZ 86005, USAOregon Institute of Technology , 3201 Campus Drive, Klamath Falls, OR 97601, USAUlugh Beg Astronomical Institute of the Uzbek Academy of Sciences , Astronomicheskaya 33, 100052 Tashkent, UzbekistanUlugh Beg Astronomical Institute of the Uzbek Academy of Sciences , Astronomicheskaya 33, 100052 Tashkent, Uzbekistan; National University of Uzbekistan , Tashkent 100174, UzbekistanUlugh Beg Astronomical Institute of the Uzbek Academy of Sciences , Astronomicheskaya 33, 100052 Tashkent, Uzbekistan; National University of Uzbekistan , Tashkent 100174, UzbekistanWe analyze variability in 15-season optical lightcurves from the doubly imaged lensed quasar SDSS J165043.44+425149.3 (SDSS1650), comprising five seasons of monitoring data from the Maidanak Observatory (277 nights in total, including the two seasons of data previously presented in Vuissoz et al.), five seasons of overlapping data from the Mercator telescope (269 nights), and 12 seasons of monitoring data from the US Naval Observatory, Flagstaff Station at lower cadence (80 nights). We update the 2007 time-delay measurement for SDSS1650 with these new data, finding a time delay of ${\rm{\Delta }}{t}_{\mathrm{AB}}=-{55.1}_{-3.7}^{+4.0}$ days, with image A leading image B. We analyze the microlensing variability in these lightcurves using a Bayesian Monte Carlo technique to yield measurements of the size of the accretion disk at λ _rest = 2420 Å, finding a half-light radius of log( r _1/2 /cm) = ${16.19}_{-0.58}^{+0.38}$ assuming a 60° inclination angle. This result is unchanged if we model 30% flux contamination from the broad-line region. We use the width of the Mg ii line in the existing Sloan Digital Sky Survey spectra to estimate the mass of this system’s supermassive black hole, finding M _BH = 2.47 × 10 ^9 M _⊙ . We confirm that the accretion disk size in this system, whose black hole mass is on the very high end of the M _BH scale, is fully consistent with the existing quasar accretion disk size–black hole mass relation.https://doi.org/10.3847/1538-4357/ad3069Quasar microlensingQuasarsGravitational lensingGravitational microlensing
spellingShingle A. B. Rivera
C. W. Morgan
S. M. Florence
K. Kniezewski
M. Millon
F. Courbin
S. E. Dahm
F. J. Vrba
T. M. Tilleman
M. A. Cornachione
I. M. Asfandiyarov
S. A. Ehgamberdiev
O. A. Burkhonov
Accretion Disk Size and Updated Time-delay Measurements in the Gravitationally Lensed Quasar SDSS J165043.44+425149.3
The Astrophysical Journal
Quasar microlensing
Quasars
Gravitational lensing
Gravitational microlensing
title Accretion Disk Size and Updated Time-delay Measurements in the Gravitationally Lensed Quasar SDSS J165043.44+425149.3
title_full Accretion Disk Size and Updated Time-delay Measurements in the Gravitationally Lensed Quasar SDSS J165043.44+425149.3
title_fullStr Accretion Disk Size and Updated Time-delay Measurements in the Gravitationally Lensed Quasar SDSS J165043.44+425149.3
title_full_unstemmed Accretion Disk Size and Updated Time-delay Measurements in the Gravitationally Lensed Quasar SDSS J165043.44+425149.3
title_short Accretion Disk Size and Updated Time-delay Measurements in the Gravitationally Lensed Quasar SDSS J165043.44+425149.3
title_sort accretion disk size and updated time delay measurements in the gravitationally lensed quasar sdss j165043 44 425149 3
topic Quasar microlensing
Quasars
Gravitational lensing
Gravitational microlensing
url https://doi.org/10.3847/1538-4357/ad3069
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