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Black Hole

Lensing of space time around a black hole. At Oxford we study black holes observationally and theoretically on all size and time scales - it is some of our core work.

Credit: ALAIN RIAZUELO, IAP/UPMC/CNRS. CLICK HERE TO VIEW MORE IMAGES.

Dr Thomas Williams

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Research theme

  • Astronomy and astrophysics

Sub department

  • Astrophysics

Research groups

  • Galaxy formation and evolution
thomas.williams@physics.ox.ac.uk
Professional Website
  • About
  • Publications

Investigating the Drivers of Electron Temperature Variations in H ii Regions with Keck-KCWI and VLT-MUSE

The Astrophysical Journal American Astronomical Society 966:1 (2024) 130

Authors:

Ryan J Rickards Vaught, Karin M Sandstrom, Francesco Belfiore, Kathryn Kreckel, J Eduardo Méndez-Delgado, Eric Emsellem, Brent Groves, Guillermo A Blanc, Daniel A Dale, Oleg V Egorov, Simon CO Glover, Kathryn Grasha, Ralf S Klessen, Justus Neumann, Thomas G Williams

Abstract:

H ii region electron temperatures are a critical ingredient in metallicity determinations, and recent observations have revealed systematic variations in the temperatures measured using different ions. We present electron temperatures (T e ) measured using the optical auroral lines ([N ii]λ5756, [O ii]λ λ7320, 7330, [S ii]λ λ4069, 4076, [O iii]λ4363, and [S iii]λ6312) for a sample of H ii regions in seven nearby galaxies. We use observations from the Physics at High Angular resolution in Nearby Galaxies survey (PHANGS) obtained with integral field spectrographs on Keck (Keck Cosmic Web Imager) and the Very Large Telescope (Multi-Unit Spectroscopic Explorer). We compare the different T e measurements with H ii region and ISM environmental properties such as electron density, ionization parameter, molecular gas velocity dispersion, and stellar association/cluster mass and age obtained from PHANGS. We find that the temperatures from [O ii] and [S ii] are likely overestimated due to the presence of electron density inhomogeneities in H ii regions. We measure high [O iii] temperatures in a subset of regions with high molecular gas velocity dispersion and low ionization parameter, which may be explained by the presence of low-velocity shocks. In agreement with previous studies, the T e–T e between [N ii] and [S iii] temperatures have the lowest observed scatter and follow predictions from photoionization modeling, which suggests that these tracers reflect H ii region temperatures across the various ionization zones better than [O ii], [S ii], and [O iii].
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WISDOM Project -- XIX. Figures of merit for supermassive black hole mass measurements using molecular gas and/or megamaser kinematics

(2024)

Authors:

Hengyue Zhang, Martin Bureau, Mark D Smith, Michele Cappellari, Timothy A Davis, Pandora Dominiak, Jacob S Elford, Fu-Heng Liang, Ilaria Ruffa, Thomas G Williams
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WISDOM Project – XIX. Figures of merit for supermassive black hole mass measurements using molecular gas and/or megamaser kinematics

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) (2024) stae1106-stae1106

Authors:

Hengyue Zhang, Martin Bureau, Mark D Smith, Michele Cappellari, Timothy A Davis, Pandora Dominiak, Jacob S Elford, Fu-Heng Liang, Ilaria Ruffa, Thomas G Williams

Abstract:

<jats:title>Abstract</jats:title> <jats:p>The mass (MBH) of a supermassive black hole (SMBH) can be measured using spatially-resolved kinematics of the region where the SMBH dominates gravitationally. The most reliable measurements are those that resolve the smallest physical scales around the SMBHs. We consider here three metrics to compare the physical scales probed by kinematic tracers dominated by rotation: the radius of the innermost detected kinematic tracer Rmin normalised by respectively the SMBH’s Schwarzschild radius (RSchw ≡ 2GMBH/c2, where G is the gravitational constant and c the speed of light), sphere-of-influence (SOI) radius ($R_\mathrm{SOI}\equiv GM_\mathrm{BH}/\sigma _\mathrm{e}^2$, where σe is the stellar velocity dispersion within the galaxy’s effective radius) and equality radius (the radius Req at which the SMBH mass equals the enclosed stellar mass, MBH = M*(Req), where M*(R) is the stellar mass enclosed within the radius R). All metrics lead to analogous simple relations between Rmin and the highest circular velocity probed Vc. Adopting these metrics to compare the SMBH mass measurements using molecular gas kinematics to those using megamaser kinematics, we demonstrate that the best molecular gas measurements resolve material that is physically closer to the SMBHs in terms of RSchw but is slightly farther in terms of RSOI and Req. However, molecular gas observations of nearby galaxies using the most extended configurations of the Atacama Large Millimeter/sub-millimeter Array can resolve the SOI comparably well and thus enable SMBH mass measurements as precise as the best megamaser measurements.</jats:p>
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The properties and kinematics of HCN emission across the closest starburst galaxy NGC 253 observed with ALMA

ArXiv 2403.13751 (2024)

Authors:

Ivana Beslic, Ashley T Barnes, Frank Bigiel, Maria Jesus Jimenez-Donaire, Antonio Usero, Jonathan D Henshaw, Christopher Faesi, Adam K Leroy, Erik Rosolowsky, Jakob S den Brok, Melanie Chevance, Cosima Eibensteiner, Kathryn Grasha, Ralf S Klessen, JM Diedrerik Kruijssen, Daizhong Liu, Sharon Meidt, Justus Neumann, Lukas Neumann, Hsi-An Pan, Johannes Puschnig, Miguel Querejeta, Eva Schinnerer, Thomas G Williams
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PHANGS Hubble Space Telescope Treasury Survey: Globular Cluster Systems in 17 Nearby Spiral Galaxies

The Astronomical Journal American Astronomical Society 167:3 (2024) 95

Authors:

Matthew Floyd, Rupali Chandar, Bradley C Whitmore, David A Thilker, Janice C Lee, Rachel E Pauline, Zion L Thomas, William J Berschback, Kiana F Henny, Daniel A Dale, Ralf S Klessen, Eva Schinnerer, Kathryn Grasha, Médéric Boquien, Kirsten L Larson, Sinan Deger, Ashley T Barnes, Adam K Leroy, Erik Rosolowsky, Thomas G Williams, Leonardo Úbeda
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