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THE HIGH-ION CONTENT AND KINEMATICS OF LOW-REDSHIFT LYMAN LIMIT SYSTEMS
We study the high-ion content and kinematics of the circumgalactic medium around low-redshift galaxies using a sample of 23 Lyman limit systems (LLSs) at 0.08 < z < 0.93 observed with the Cosmic Origins Spectrograph on board the Hubble Space Telescope. In Lehner et al., we recently showed that...
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Published in: | The Astrophysical journal 2013-12, Vol.778 (2), p.1-16 |
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creator | Fox, Andrew J Lehner, Nicolas Tumlinson, Jason Howk, J Christopher Tripp, Todd M Prochaska, J Xavier O'Meara, John M Werk, Jessica K BORDOLOI, RONGMON Katz, Neal Oppenheimer, Benjamin D Dave, Romeel |
description | We study the high-ion content and kinematics of the circumgalactic medium around low-redshift galaxies using a sample of 23 Lyman limit systems (LLSs) at 0.08 < z < 0.93 observed with the Cosmic Origins Spectrograph on board the Hubble Space Telescope. In Lehner et al., we recently showed that low-z LLSs have a bimodal metallicity distribution. Here we extend that analysis to search for differences between the high-ion and kinematic properties of the metal-poor and metal-rich branches. We find that metal-rich LLSs tend to show higher O VI columns and broader O VI profiles than metal-poor LLSs. The total H I line width ( Delta v sub(90) statistic) in LLSs is not correlated with metallicity, indicating that the HI kinematics alone cannot be used to distinguish inflow from outflow and gas recycling. Among the 17 LLSs with O VI detections, all but two show evidence of kinematic sub-structure, in the form of O VI-H I centroid offsets, multiple components, or both. Using various scenarios for how the metallicities in the high-ion and low-ion phases of each LLS compare, we constrain the ionized hydrogen column in the O VI phase to lie in the range log N(H II) similar to 17.6-20. The O VI phase of LLSs is a substantial baryon reservoir, with M(high-ion) similar to 10 super(8.5-10.9) (r/150 kpc) super(2) M sub([middot in circle]), similar to the mass in the low-ion phase. Accounting for the O VI phase approximately doubles the contribution of low-z LLSs to the cosmic baryon budget. |
doi_str_mv | 10.1088/0004-637X/778/2/187 |
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In Lehner et al., we recently showed that low-z LLSs have a bimodal metallicity distribution. Here we extend that analysis to search for differences between the high-ion and kinematic properties of the metal-poor and metal-rich branches. We find that metal-rich LLSs tend to show higher O VI columns and broader O VI profiles than metal-poor LLSs. The total H I line width ( Delta v sub(90) statistic) in LLSs is not correlated with metallicity, indicating that the HI kinematics alone cannot be used to distinguish inflow from outflow and gas recycling. Among the 17 LLSs with O VI detections, all but two show evidence of kinematic sub-structure, in the form of O VI-H I centroid offsets, multiple components, or both. Using various scenarios for how the metallicities in the high-ion and low-ion phases of each LLS compare, we constrain the ionized hydrogen column in the O VI phase to lie in the range log N(H II) similar to 17.6-20. The O VI phase of LLSs is a substantial baryon reservoir, with M(high-ion) similar to 10 super(8.5-10.9) (r/150 kpc) super(2) M sub([middot in circle]), similar to the mass in the low-ion phase. 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In Lehner et al., we recently showed that low-z LLSs have a bimodal metallicity distribution. Here we extend that analysis to search for differences between the high-ion and kinematic properties of the metal-poor and metal-rich branches. We find that metal-rich LLSs tend to show higher O VI columns and broader O VI profiles than metal-poor LLSs. The total H I line width ( Delta v sub(90) statistic) in LLSs is not correlated with metallicity, indicating that the HI kinematics alone cannot be used to distinguish inflow from outflow and gas recycling. Among the 17 LLSs with O VI detections, all but two show evidence of kinematic sub-structure, in the form of O VI-H I centroid offsets, multiple components, or both. Using various scenarios for how the metallicities in the high-ion and low-ion phases of each LLS compare, we constrain the ionized hydrogen column in the O VI phase to lie in the range log N(H II) similar to 17.6-20. The O VI phase of LLSs is a substantial baryon reservoir, with M(high-ion) similar to 10 super(8.5-10.9) (r/150 kpc) super(2) M sub([middot in circle]), similar to the mass in the low-ion phase. Accounting for the O VI phase approximately doubles the contribution of low-z LLSs to the cosmic baryon budget.</description><subject>APPROXIMATIONS</subject><subject>ASTROPHYSICS, COSMOLOGY AND ASTRONOMY</subject><subject>BARYONS</subject><subject>COMPARATIVE EVALUATIONS</subject><subject>DETECTION</subject><subject>DISTRIBUTION</subject><subject>GALAXIES</subject><subject>Hubble Space Telescope</subject><subject>HYDROGEN</subject><subject>Kinematics</subject><subject>LINE WIDTHS</subject><subject>MASS</subject><subject>METALLICITY</subject><subject>METALS</subject><subject>Phases</subject><subject>RED SHIFT</subject><subject>Samples</subject><subject>Searching</subject><subject>SPACE</subject><subject>Statistical methods</subject><subject>TELESCOPES</subject><issn>0004-637X</issn><issn>1538-4357</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2013</creationdate><recordtype>article</recordtype><recordid>eNqNkU9LwzAYh4MoOKefwEvAi5fapGmb5Fi2bg32D9iI7hRilmJlW7XpDn57WyaePb28vA8_eH8PALcYPWDEmI8QCr2Y0FefUuYHPmb0DMxwRJgXkoieg9kfcQmunPuY1oDzGVjLLIWZWGeeqEq4qEqZlhIm5RI-ijItEikWNaxWMK9evKd0WWdiJWG-KZIS5qIQEtabWqZFfQ0uGr1z9uZ3zsHzKpWLzMurtVgkuWcIY4NnbKCx0biJKH_DDY1CFhndoJjgmBJuMUIMs5DEDds22GwR1kgjPp5is40ZJXNwd8rt3NAqZ9rBmnfTHQ7WDCoISIj5-PYc3J-oz777Olo3qH3rjN3t9MF2R6cwxYyTiNH4HyiKEI0o5SNKTqjpO-d626jPvt3r_lthpCYPaqpVTS2r0YMK1OiB_AADH3Iz</recordid><startdate>20131201</startdate><enddate>20131201</enddate><creator>Fox, Andrew J</creator><creator>Lehner, Nicolas</creator><creator>Tumlinson, Jason</creator><creator>Howk, J Christopher</creator><creator>Tripp, Todd M</creator><creator>Prochaska, J Xavier</creator><creator>O'Meara, John M</creator><creator>Werk, Jessica K</creator><creator>BORDOLOI, RONGMON</creator><creator>Katz, Neal</creator><creator>Oppenheimer, Benjamin D</creator><creator>Dave, Romeel</creator><scope>AAYXX</scope><scope>CITATION</scope><scope>7TG</scope><scope>KL.</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>OTOTI</scope></search><sort><creationdate>20131201</creationdate><title>THE HIGH-ION CONTENT AND KINEMATICS OF LOW-REDSHIFT LYMAN LIMIT SYSTEMS</title><author>Fox, Andrew J ; Lehner, Nicolas ; Tumlinson, Jason ; Howk, J Christopher ; Tripp, Todd M ; Prochaska, J Xavier ; O'Meara, John M ; Werk, Jessica K ; BORDOLOI, RONGMON ; Katz, Neal ; Oppenheimer, Benjamin D ; Dave, Romeel</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c388t-ce2a1ca1f579b1f75485caf06316739e100818436f8df1cd01a0a097396cd6873</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2013</creationdate><topic>APPROXIMATIONS</topic><topic>ASTROPHYSICS, COSMOLOGY AND ASTRONOMY</topic><topic>BARYONS</topic><topic>COMPARATIVE EVALUATIONS</topic><topic>DETECTION</topic><topic>DISTRIBUTION</topic><topic>GALAXIES</topic><topic>Hubble Space Telescope</topic><topic>HYDROGEN</topic><topic>Kinematics</topic><topic>LINE WIDTHS</topic><topic>MASS</topic><topic>METALLICITY</topic><topic>METALS</topic><topic>Phases</topic><topic>RED SHIFT</topic><topic>Samples</topic><topic>Searching</topic><topic>SPACE</topic><topic>Statistical methods</topic><topic>TELESCOPES</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Fox, Andrew J</creatorcontrib><creatorcontrib>Lehner, Nicolas</creatorcontrib><creatorcontrib>Tumlinson, Jason</creatorcontrib><creatorcontrib>Howk, J Christopher</creatorcontrib><creatorcontrib>Tripp, Todd M</creatorcontrib><creatorcontrib>Prochaska, J Xavier</creatorcontrib><creatorcontrib>O'Meara, John M</creatorcontrib><creatorcontrib>Werk, Jessica K</creatorcontrib><creatorcontrib>BORDOLOI, RONGMON</creatorcontrib><creatorcontrib>Katz, Neal</creatorcontrib><creatorcontrib>Oppenheimer, Benjamin D</creatorcontrib><creatorcontrib>Dave, Romeel</creatorcontrib><collection>CrossRef</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>OSTI.GOV</collection><jtitle>The Astrophysical journal</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Fox, Andrew J</au><au>Lehner, Nicolas</au><au>Tumlinson, Jason</au><au>Howk, J Christopher</au><au>Tripp, Todd M</au><au>Prochaska, J Xavier</au><au>O'Meara, John M</au><au>Werk, Jessica K</au><au>BORDOLOI, RONGMON</au><au>Katz, Neal</au><au>Oppenheimer, Benjamin D</au><au>Dave, Romeel</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>THE HIGH-ION CONTENT AND KINEMATICS OF LOW-REDSHIFT LYMAN LIMIT SYSTEMS</atitle><jtitle>The Astrophysical journal</jtitle><date>2013-12-01</date><risdate>2013</risdate><volume>778</volume><issue>2</issue><spage>1</spage><epage>16</epage><pages>1-16</pages><issn>0004-637X</issn><eissn>1538-4357</eissn><abstract>We study the high-ion content and kinematics of the circumgalactic medium around low-redshift galaxies using a sample of 23 Lyman limit systems (LLSs) at 0.08 < z < 0.93 observed with the Cosmic Origins Spectrograph on board the Hubble Space Telescope. In Lehner et al., we recently showed that low-z LLSs have a bimodal metallicity distribution. Here we extend that analysis to search for differences between the high-ion and kinematic properties of the metal-poor and metal-rich branches. We find that metal-rich LLSs tend to show higher O VI columns and broader O VI profiles than metal-poor LLSs. The total H I line width ( Delta v sub(90) statistic) in LLSs is not correlated with metallicity, indicating that the HI kinematics alone cannot be used to distinguish inflow from outflow and gas recycling. Among the 17 LLSs with O VI detections, all but two show evidence of kinematic sub-structure, in the form of O VI-H I centroid offsets, multiple components, or both. Using various scenarios for how the metallicities in the high-ion and low-ion phases of each LLS compare, we constrain the ionized hydrogen column in the O VI phase to lie in the range log N(H II) similar to 17.6-20. The O VI phase of LLSs is a substantial baryon reservoir, with M(high-ion) similar to 10 super(8.5-10.9) (r/150 kpc) super(2) M sub([middot in circle]), similar to the mass in the low-ion phase. Accounting for the O VI phase approximately doubles the contribution of low-z LLSs to the cosmic baryon budget.</abstract><cop>United States</cop><doi>10.1088/0004-637X/778/2/187</doi><tpages>16</tpages><oa>free_for_read</oa></addata></record> |
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subjects | APPROXIMATIONS ASTROPHYSICS, COSMOLOGY AND ASTRONOMY BARYONS COMPARATIVE EVALUATIONS DETECTION DISTRIBUTION GALAXIES Hubble Space Telescope HYDROGEN Kinematics LINE WIDTHS MASS METALLICITY METALS Phases RED SHIFT Samples Searching SPACE Statistical methods TELESCOPES |
title | THE HIGH-ION CONTENT AND KINEMATICS OF LOW-REDSHIFT LYMAN LIMIT SYSTEMS |
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