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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
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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 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 (2016)

Authors:

Martin Bureau, Alfred L Tiley, 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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KROSS: Mapping the Ha emission across the star-formation sequence at z~1

Monthly Notices Of The Royal Astronomical Society Oxford University Press 456:4 (2016) 4533-4541

Authors:

Georgios E Magdis, Martin Bureau, JP Stott, A Tiley, AM Swinbank, R Bower, AJ Bunker, Matthew Jarvis, H Johnson, R Sharples

Abstract:

We present first results from the KMOS Redshift One Spectroscopic Survey (KROSS), an ongoing large kinematical survey of a thousand, z~1 star forming galaxies, with VLT KMOS. Out of the targeted galaxies (~500 so far), we detect and spatially resolve Ha emission in ~90% and 77% of the sample respectively. Based on the integrated Ha flux measurements and the spatially resolved maps we derive a median star formation rate (SFR) of ~7.0 Msun/yr and a median physical size of = 5.1kpc. We combine the inferred SFRs and effective radii measurements to derive the star formation surface densities ({\Sigma}SFR) and present a "resolved" version of the star formation main sequence (MS) that appears to hold at sub-galactic scales, with similar slope and scatter as the one inferred from galaxy integrated properties. Our data also yield a trend between {\Sigma}SFR and {\Delta}(sSFR) (distance from the MS) suggesting that galaxies with higher sSFR are characterised by denser star formation activity. Similarly, we find evidence for an anti-correlation between the gas phase metallicity (Z) and the {\Delta}(sSFR), suggesting a 0.2dex variation in the metal content of galaxies within the MS and significantly lower metallicities for galaxies above it. The origin of the observed trends between {\Sigma}SFR - {\Sigma}(sSFR) and Z - {\Delta}(sSFR) could be driven by an interplay between variations of the gas fraction or the star formation efficiency of the galaxies along and off the MS. To address this, follow-up observations of the our sample that will allow gas mass estimates are necessary.
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