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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.

Martin Bureau

Professor of Astrophysics

Research theme

  • Astronomy and astrophysics

Sub department

  • Astrophysics

Research groups

  • Galaxy formation and evolution
  • Hintze Centre for Astrophysical Surveys
martin.bureau@physics.ox.ac.uk
Telephone: 01865 (2)73377
Denys Wilkinson Building, room 701
Home page
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  • About
  • Publications

Black Hole Mass Measurement in Nearby Galaxy Using Molecular Gas Dynamics

Institute of Electrical and Electronics Engineers (IEEE) (2016) 1-4

Authors:

Kyoko Onishi, Satoru Iguchi, Timothy Davis, Martin Bureau, Michele Cappellari, Leo Blitz, Marc Sarzi
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The KMOS Redshift One Spectroscopic Survey (KROSS): the Tully-Fisher relation at z similar to 1

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY 460:1 (2016) 103-129

Authors:

AL Tiley, JP Stott, AM Swinbank, M Bureau, CM Harrison, R Bower, HL Johnson, AJ Bunker, MJ Jarvis, G Magdis, R Sharples, I Smail, D Sobral, P Best
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The Tully-Fisher Relation of COLD GASS Galaxies

(2016)

Authors:

Alfred L Tiley, Martin Bureau, Amélie Saintonge, Selcuk Topal, Timothy A Davis, Kazufumi Torii
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The Tully-Fisher relation of COLD GASS galaxies

Monthly Notices of the Royal Astronomical Society Oxford University Press 461:4 (2016) 3494-3515

Authors:

Alfred L Tiley, Martin Bureau, Amélie Saintonge, Selcuk Topal, Timothy A Davis, Kazufumi Torii

Abstract:

We present the stellar mass (M*) and Wide-Field Infrared Survey Explorer (WISE) absolute Band 1 magnitude (MW1) Tully-Fisher relations (TFRs) of subsets of galaxies from the CO Legacy Database for the Galex Arecibo SDSS Survey (COLD GASS). We examine the benefits and drawbacks of several commonly used fitting functions in the context of measuring CO(1-0) line widths (and thus rotation velocities), favouring the Gaussian Double Peak function. We find the MW1 and M* TFR, for a carefully selected sub-sample, to be MW1 = (-7.1 ± 0.6) [log(W50/sin i / km s^-1) - 23.83 ± 0.09 and log (M*/M⊙) = (3.3 ± 0.3) [log(W50/sin i / km s^-1) -2.58] + 10:51 ± 0.04, respectively, where W50 is the width of a galaxy's CO(1-0) integrated profile at 50% of its maximum and the inclination i is derived from the galaxy axial ratio measured on the SDSS r-band image. We find no evidence for any significant offset between the TFRs of COLD GASS galaxies and those of comparison samples of similar redshifts and morphologies. The slope of the COLD GASS M* TFR agrees with the relation of Pizagno et al. (2005). However, we measure a comparitively shallower slope for the COLD GASS MW1 TFR as compared to the relation of Tully and Pierce (2000). We attribute this to the fact that the COLD GASS sample comprises galaxies of various (late-type) morphologies. Nevertheless, our work provides a robust reference point with which to compare future CO TFR studies.
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The KMOS Redshift One Spectroscopic Survey (KROSS): The Tully-Fisher Relation at z ~ 1

(2016)

Authors:

Alfred L Tiley, John P Stott, AM Swinbank, Martin Bureau, Chris M Harrison, Richard Bower, Helen L Johnson, Andrew J Bunker, Matt J Jarvis, Georgios Magdis, Ray Sharples, Ian Smail, David Sobral, Philip Best
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