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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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 |
format | Article |
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$=7.6^{+2.0}_{-1.6}$
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.</description><identifier>ISSN: 0035-8711</identifier><identifier>EISSN: 1365-2966</identifier><identifier>DOI: 10.1093/mnras/stv389</identifier><language>eng</language><publisher>London: Oxford University Press</publisher><subject>Astronomy ; Elevated ; Hubble Space Telescope ; Imaging ; Kinematics ; Luminosity ; Mass ratios ; Mathematical models ; Searching ; Spectroscopy ; Star & galaxy formation ; Stellar populations ; Stripping ; Velocity</subject><ispartof>Monthly notices of the Royal Astronomical Society, 2015-05, Vol.449 (2), p.1716-1730</ispartof><rights>2015 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society 2015</rights><rights>Copyright Oxford University Press, UK May 11, 2015</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c399t-a3c7e80a4967dd25b9a383c730363289a8f6288a9b4d7511e2edbb0aec47ec0b3</citedby><cites>FETCH-LOGICAL-c399t-a3c7e80a4967dd25b9a383c730363289a8f6288a9b4d7511e2edbb0aec47ec0b3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,1604,27924,27925</link.rule.ids><linktorsrc>$$Uhttps://dx.doi.org/10.1093/mnras/stv389$$EView_record_in_Oxford_University_Press$$FView_record_in_$$GOxford_University_Press</linktorsrc></links><search><creatorcontrib>Janz, Joachim</creatorcontrib><creatorcontrib>Forbes, Duncan A.</creatorcontrib><creatorcontrib>Norris, Mark A.</creatorcontrib><creatorcontrib>Strader, Jay</creatorcontrib><creatorcontrib>Penny, Samantha J.</creatorcontrib><creatorcontrib>Fagioli, Martina</creatorcontrib><creatorcontrib>Romanowsky, Aaron J.</creatorcontrib><title>How elevated is the dynamical-to-stellar mass ratio of the ultracompact dwarf S999?</title><title>Monthly notices of the Royal Astronomical Society</title><addtitle>Mon. Not. R. Astron. Soc</addtitle><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.</description><subject>Astronomy</subject><subject>Elevated</subject><subject>Hubble Space Telescope</subject><subject>Imaging</subject><subject>Kinematics</subject><subject>Luminosity</subject><subject>Mass ratios</subject><subject>Mathematical models</subject><subject>Searching</subject><subject>Spectroscopy</subject><subject>Star & galaxy formation</subject><subject>Stellar populations</subject><subject>Stripping</subject><subject>Velocity</subject><issn>0035-8711</issn><issn>1365-2966</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNqN0c9LwzAUB_AgCs7pzT8g4EEP1r0kbZqcRIa_YOBhei6vaYod7TKTdGP_vd3myYN4evD48Pg-voRcMrhjoMWkW3oMkxDXQukjMmJCZgnXUh6TEYDIEpUzdkrOQlgAQCq4HJH5i9tQ29o1RlvRJtD4aWm1XWLXGGyT6JIQbduipx2GQD3GxlFX71nfRo_GdSs0kVYb9DWda63vz8lJjW2wFz9zTD6eHt-nL8ns7fl1-jBLjNA6JihMbhVgqmVeVTwrNQo17AQIKbjSqGrJlUJdplWeMWa5rcoS0Jo0twZKMSY3h7sr7756G2LRNcHs0i6t60PBpMoUqBT4fyikGZcZDPTqF1243i-HRwaVDwm5VGxQtwdlvAvB27pY-aZDvy0YFLsyin0ZxaGMgV8fuOtXf8tvCyCLCg</recordid><startdate>20150511</startdate><enddate>20150511</enddate><creator>Janz, Joachim</creator><creator>Forbes, Duncan A.</creator><creator>Norris, Mark A.</creator><creator>Strader, Jay</creator><creator>Penny, Samantha J.</creator><creator>Fagioli, Martina</creator><creator>Romanowsky, Aaron J.</creator><general>Oxford University Press</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>7TG</scope><scope>KL.</scope></search><sort><creationdate>20150511</creationdate><title>How elevated is the dynamical-to-stellar mass ratio of the ultracompact dwarf S999?</title><author>Janz, Joachim ; Forbes, Duncan A. ; Norris, Mark A. ; Strader, Jay ; Penny, Samantha J. ; Fagioli, Martina ; Romanowsky, Aaron J.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c399t-a3c7e80a4967dd25b9a383c730363289a8f6288a9b4d7511e2edbb0aec47ec0b3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>Astronomy</topic><topic>Elevated</topic><topic>Hubble Space Telescope</topic><topic>Imaging</topic><topic>Kinematics</topic><topic>Luminosity</topic><topic>Mass ratios</topic><topic>Mathematical models</topic><topic>Searching</topic><topic>Spectroscopy</topic><topic>Star & galaxy formation</topic><topic>Stellar populations</topic><topic>Stripping</topic><topic>Velocity</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Janz, Joachim</creatorcontrib><creatorcontrib>Forbes, Duncan A.</creatorcontrib><creatorcontrib>Norris, Mark A.</creatorcontrib><creatorcontrib>Strader, Jay</creatorcontrib><creatorcontrib>Penny, Samantha J.</creatorcontrib><creatorcontrib>Fagioli, Martina</creatorcontrib><creatorcontrib>Romanowsky, Aaron J.</creatorcontrib><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><jtitle>Monthly notices of the Royal Astronomical Society</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Janz, Joachim</au><au>Forbes, Duncan A.</au><au>Norris, Mark A.</au><au>Strader, Jay</au><au>Penny, Samantha J.</au><au>Fagioli, Martina</au><au>Romanowsky, Aaron J.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>How elevated is the dynamical-to-stellar mass ratio of the ultracompact dwarf S999?</atitle><jtitle>Monthly notices of the Royal Astronomical Society</jtitle><stitle>Mon. 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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