How elevated is the dynamical-to-stellar mass ratio of the ultracompact dwarf S999?

Here we present new Keck Echelle Spectrograph and Imager high-resolution spectroscopy and deep archival Hubble Space Telescope/Advanced Camera for Surveys imaging for S999, an ultracompact dwarf in the vicinity of M87, which was claimed to have an extremely high dynamical-to-stellar mass ratio. Our...

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Veröffentlicht in:Monthly notices of the Royal Astronomical Society 2015-05, Vol.449 (2), p.1716-1730
Hauptverfasser: Janz, Joachim, Forbes, Duncan A., Norris, Mark A., Strader, Jay, Penny, Samantha J., Fagioli, Martina, Romanowsky, Aaron J.
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container_end_page 1730
container_issue 2
container_start_page 1716
container_title Monthly notices of the Royal Astronomical Society
container_volume 449
creator Janz, Joachim
Forbes, Duncan A.
Norris, Mark A.
Strader, Jay
Penny, Samantha J.
Fagioli, Martina
Romanowsky, Aaron J.
description Here we present new Keck Echelle Spectrograph and Imager high-resolution spectroscopy and deep archival Hubble Space Telescope/Advanced Camera for Surveys imaging for S999, an ultracompact dwarf in the vicinity of M87, which was claimed to have an extremely high dynamical-to-stellar mass ratio. Our data increase the total integration times by a factor of 5 and 60 for spectroscopy and imaging, respectively. This allows us to constrain the stellar population parameters for the first time (simple stellar population equivalent age $=7.6^{+2.0}_{-1.6}$  Gyr; $[Z/\textrm {H}]=-0.95^{+0.12}_{-0.10}$ ; $[\alpha /\textrm {Fe}]=0.34^{+0.10}_{-0.12}$ ). Assuming a Kroupa stellar initial mass function, the stellar population parameters and luminosity (M F814W  = −12.13 ± 0.06 mag) yield a stellar mass of $M_*=3.9^{+0.9}_{-0.6}\times 10^6\,\mathrm{M}_{{\odot }}$ , which we also find to be consistent with near-infrared data. Via mass modelling, with our new measurements of velocity dispersion (σap = 27 ± 2 km s−1) and size (R e = 20.9 ± 1.0 pc), we obtain an elevated dynamical-to-stellar mass ratio M dyn/M * = 8.2 (with a range 5.6 ≤ M dyn/M * ≤ 11.2). Furthermore, we analyse the surface brightness profile of S999, finding only a small excess of light in the outer parts with respect to the fitted Sérsic profile, and a positive colour gradient. Taken together these observations suggest that S999 is the remnant of a much larger galaxy that has been tidally stripped. If so, the observed elevated mass ratio may be caused by mechanisms related to the stripping process: the existence of a massive central black hole or internal kinematics that are out of equilibrium due to the stripping event. Given the observed dynamical-to-stellar mass ratio we suggest that S999 is an ideal candidate to search for the presence of an overly massive central black hole.
doi_str_mv 10.1093/mnras/stv389
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Our data increase the total integration times by a factor of 5 and 60 for spectroscopy and imaging, respectively. This allows us to constrain the stellar population parameters for the first time (simple stellar population equivalent age $=7.6^{+2.0}_{-1.6}$  Gyr; $[Z/\textrm {H}]=-0.95^{+0.12}_{-0.10}$ ; $[\alpha /\textrm {Fe}]=0.34^{+0.10}_{-0.12}$ ). Assuming a Kroupa stellar initial mass function, the stellar population parameters and luminosity (M F814W  = −12.13 ± 0.06 mag) yield a stellar mass of $M_*=3.9^{+0.9}_{-0.6}\times 10^6\,\mathrm{M}_{{\odot }}$ , which we also find to be consistent with near-infrared data. Via mass modelling, with our new measurements of velocity dispersion (σap = 27 ± 2 km s−1) and size (R e = 20.9 ± 1.0 pc), we obtain an elevated dynamical-to-stellar mass ratio M dyn/M * = 8.2 (with a range 5.6 ≤ M dyn/M * ≤ 11.2). Furthermore, we analyse the surface brightness profile of S999, finding only a small excess of light in the outer parts with respect to the fitted Sérsic profile, and a positive colour gradient. Taken together these observations suggest that S999 is the remnant of a much larger galaxy that has been tidally stripped. If so, the observed elevated mass ratio may be caused by mechanisms related to the stripping process: the existence of a massive central black hole or internal kinematics that are out of equilibrium due to the stripping event. 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Via mass modelling, with our new measurements of velocity dispersion (σap = 27 ± 2 km s−1) and size (R e = 20.9 ± 1.0 pc), we obtain an elevated dynamical-to-stellar mass ratio M dyn/M * = 8.2 (with a range 5.6 ≤ M dyn/M * ≤ 11.2). Furthermore, we analyse the surface brightness profile of S999, finding only a small excess of light in the outer parts with respect to the fitted Sérsic profile, and a positive colour gradient. Taken together these observations suggest that S999 is the remnant of a much larger galaxy that has been tidally stripped. If so, the observed elevated mass ratio may be caused by mechanisms related to the stripping process: the existence of a massive central black hole or internal kinematics that are out of equilibrium due to the stripping event. 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Not. R. Astron. Soc</stitle><date>2015-05-11</date><risdate>2015</risdate><volume>449</volume><issue>2</issue><spage>1716</spage><epage>1730</epage><pages>1716-1730</pages><issn>0035-8711</issn><eissn>1365-2966</eissn><abstract>Here we present new Keck Echelle Spectrograph and Imager high-resolution spectroscopy and deep archival Hubble Space Telescope/Advanced Camera for Surveys imaging for S999, an ultracompact dwarf in the vicinity of M87, which was claimed to have an extremely high dynamical-to-stellar mass ratio. Our data increase the total integration times by a factor of 5 and 60 for spectroscopy and imaging, respectively. This allows us to constrain the stellar population parameters for the first time (simple stellar population equivalent age $=7.6^{+2.0}_{-1.6}$  Gyr; $[Z/\textrm {H}]=-0.95^{+0.12}_{-0.10}$ ; $[\alpha /\textrm {Fe}]=0.34^{+0.10}_{-0.12}$ ). Assuming a Kroupa stellar initial mass function, the stellar population parameters and luminosity (M F814W  = −12.13 ± 0.06 mag) yield a stellar mass of $M_*=3.9^{+0.9}_{-0.6}\times 10^6\,\mathrm{M}_{{\odot }}$ , which we also find to be consistent with near-infrared data. Via mass modelling, with our new measurements of velocity dispersion (σap = 27 ± 2 km s−1) and size (R e = 20.9 ± 1.0 pc), we obtain an elevated dynamical-to-stellar mass ratio M dyn/M * = 8.2 (with a range 5.6 ≤ M dyn/M * ≤ 11.2). Furthermore, we analyse the surface brightness profile of S999, finding only a small excess of light in the outer parts with respect to the fitted Sérsic profile, and a positive colour gradient. Taken together these observations suggest that S999 is the remnant of a much larger galaxy that has been tidally stripped. If so, the observed elevated mass ratio may be caused by mechanisms related to the stripping process: the existence of a massive central black hole or internal kinematics that are out of equilibrium due to the stripping event. Given the observed dynamical-to-stellar mass ratio we suggest that S999 is an ideal candidate to search for the presence of an overly massive central black hole.</abstract><cop>London</cop><pub>Oxford University Press</pub><doi>10.1093/mnras/stv389</doi><tpages>15</tpages><oa>free_for_read</oa></addata></record>
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subjects Astronomy
Elevated
Hubble Space Telescope
Imaging
Kinematics
Luminosity
Mass ratios
Mathematical models
Searching
Spectroscopy
Star & galaxy formation
Stellar populations
Stripping
Velocity
title How elevated is the dynamical-to-stellar mass ratio of the ultracompact dwarf S999?
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