The Tully–Fisher relation of COLD GASS Galaxies

We present the stellar mass (M *) and Wide-Field Infrared Survey Explorer absolute Band 1 magnitude (M W1) 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 fi...

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Veröffentlicht in:Monthly notices of the Royal Astronomical Society 2016-10, Vol.461 (4), p.3494-3515
Hauptverfasser: Tiley, Alfred L., Bureau, Martin, Saintonge, Amélie, Topal, Selcuk, Davis, Timothy A., Torii, Kazufumi
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container_end_page 3515
container_issue 4
container_start_page 3494
container_title Monthly notices of the Royal Astronomical Society
container_volume 461
creator Tiley, Alfred L.
Bureau, Martin
Saintonge, Amélie
Topal, Selcuk
Davis, Timothy A.
Torii, Kazufumi
description We present the stellar mass (M *) and Wide-Field Infrared Survey Explorer absolute Band 1 magnitude (M W1) 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) linewidths (and thus rotation velocities), favouring the Gaussian Double Peak function. We find the M W1 and M * TFR, for a carefully selected sub-sample, to be $M_{W1} = (-7.1\pm 0.6) [\log {(\frac{W_{50}/\sin {i}}{{\rm km\,s}^{-1}})}-2.58] - 23.83 \pm 0.09$ and $\log {(M_{{\ast }}/\mathrm{M}_{{\odot }})} = (3.3\pm 0.3) [\log {(\frac{W_{50}{/}\sin {i}}{{\rm km\,s}^{-1}})}-2.58] + 10.51\pm 0.04$ , respectively, where W 50 is the width of a galaxy's CO(1–0) integrated profile at 50 per cent of its maximum and the inclination i is derived from the galaxy axial ratio measured on the Sloan Digitized Sky Survey 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. However, we measure a comparatively shallower slope for the COLD GASS M W1 TFR as compared to the relation of Tully & Pierce. 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.
doi_str_mv 10.1093/mnras/stw1545
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We examine the benefits and drawbacks of several commonly used fitting functions in the context of measuring CO(1–0) linewidths (and thus rotation velocities), favouring the Gaussian Double Peak function. We find the M W1 and M * TFR, for a carefully selected sub-sample, to be $M_{W1} = (-7.1\pm 0.6) [\log {(\frac{W_{50}/\sin {i}}{{\rm km\,s}^{-1}})}-2.58] - 23.83 \pm 0.09$ and $\log {(M_{{\ast }}/\mathrm{M}_{{\odot }})} = (3.3\pm 0.3) [\log {(\frac{W_{50}{/}\sin {i}}{{\rm km\,s}^{-1}})}-2.58] + 10.51\pm 0.04$ , respectively, where W 50 is the width of a galaxy's CO(1–0) integrated profile at 50 per cent of its maximum and the inclination i is derived from the galaxy axial ratio measured on the Sloan Digitized Sky Survey 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. 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We examine the benefits and drawbacks of several commonly used fitting functions in the context of measuring CO(1–0) linewidths (and thus rotation velocities), favouring the Gaussian Double Peak function. We find the M W1 and M * TFR, for a carefully selected sub-sample, to be $M_{W1} = (-7.1\pm 0.6) [\log {(\frac{W_{50}/\sin {i}}{{\rm km\,s}^{-1}})}-2.58] - 23.83 \pm 0.09$ and $\log {(M_{{\ast }}/\mathrm{M}_{{\odot }})} = (3.3\pm 0.3) [\log {(\frac{W_{50}{/}\sin {i}}{{\rm km\,s}^{-1}})}-2.58] + 10.51\pm 0.04$ , respectively, where W 50 is the width of a galaxy's CO(1–0) integrated profile at 50 per cent of its maximum and the inclination i is derived from the galaxy axial ratio measured on the Sloan Digitized Sky Survey 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. 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We examine the benefits and drawbacks of several commonly used fitting functions in the context of measuring CO(1–0) linewidths (and thus rotation velocities), favouring the Gaussian Double Peak function. We find the M W1 and M * TFR, for a carefully selected sub-sample, to be $M_{W1} = (-7.1\pm 0.6) [\log {(\frac{W_{50}/\sin {i}}{{\rm km\,s}^{-1}})}-2.58] - 23.83 \pm 0.09$ and $\log {(M_{{\ast }}/\mathrm{M}_{{\odot }})} = (3.3\pm 0.3) [\log {(\frac{W_{50}{/}\sin {i}}{{\rm km\,s}^{-1}})}-2.58] + 10.51\pm 0.04$ , respectively, where W 50 is the width of a galaxy's CO(1–0) integrated profile at 50 per cent of its maximum and the inclination i is derived from the galaxy axial ratio measured on the Sloan Digitized Sky Survey 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. However, we measure a comparatively shallower slope for the COLD GASS M W1 TFR as compared to the relation of Tully &amp; Pierce. 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.</abstract><cop>London</cop><pub>Oxford University Press</pub><doi>10.1093/mnras/stw1545</doi><tpages>22</tpages><oa>free_for_read</oa></addata></record>
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subjects Astrophysics
Comparative analysis
Cosmology
Galaxies
Gaussian
Inclination
Legacy
Mathematical functions
Morphology
Normal distribution
Red shift
Slopes
Star & galaxy formation
Wide-field Infrared Survey Explorer
title The Tully–Fisher relation of COLD GASS Galaxies
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