MEASURING QUASAR VARIABILITY WITH Pan-STARRS1 AND SDSS
We measure quasar variability using the Panoramic Survey Telescope and Rapid Response System 1 Survey (Pan-STARRS1 or PS1) and the Sloan Digital Sky Survey (SDSS) and establish a method of selecting quasars via their variability in 10 super(4) deg super(2) surveys. We use 10 super(5) spectroscopical...
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Veröffentlicht in: | The Astrophysical journal 2014-04, Vol.784 (2), p.1-16 |
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creator | Morganson, E Burgett, W S Chambers, K C Green, P J Kaiser, N Magnier, E A Marshall, P J Morgan, J S Price, P A Rix, H-W Schlafly, E F Tonry, J L Walter, F |
description | We measure quasar variability using the Panoramic Survey Telescope and Rapid Response System 1 Survey (Pan-STARRS1 or PS1) and the Sloan Digital Sky Survey (SDSS) and establish a method of selecting quasars via their variability in 10 super(4) deg super(2) surveys. We use 10 super(5) spectroscopically confirmed quasars that have been well measured in both PSI and SDSS and take advantage of the decadal timescales that separate SDSS measurements and PS1 measurements. A power law model fits the data well over the entire time range tested, 0.01-10 yr. Variability in the current PS1-SDSS data set can efficiently distinguish between quasars and nonvarying objects. It improves the purity of a griz quasar color cut from 4.1% to 48% while maintaining 67% completeness. Variability will be very effective at finding quasars in data sets with no u band and in redshift ranges where exclusively photometric selection is not efficient. We show that quasars' rest-frame ensemble variability, measured as a root mean squared in [Delta] magnitudes, is consistent with V(z, L, t) = A sub(0)(1 + z) super(0.37)(L/L sub(0)) super(-0.16)(t/1 yr) super(0.246), where L sub(0) = 10 super(46) erg s super(-1) and A sub(0) = 0.190, 0.162, 0.147, or 0.141 in the g sub(P1), r sub(P1), i sub(P1), or z sub(P1) filter, respectively. We also fit across all four filters and obtain median variability as a function of z, L, and [lambda] as V(z, L, [lambda], t) = 0.079(1 + z) super(0.15)(L/L sub(0)) super(-0.2)([lambda]/1000nm) super(-0.44)(t /1 yr) super(0.246). |
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We use 10 super(5) spectroscopically confirmed quasars that have been well measured in both PSI and SDSS and take advantage of the decadal timescales that separate SDSS measurements and PS1 measurements. A power law model fits the data well over the entire time range tested, 0.01-10 yr. Variability in the current PS1-SDSS data set can efficiently distinguish between quasars and nonvarying objects. It improves the purity of a griz quasar color cut from 4.1% to 48% while maintaining 67% completeness. Variability will be very effective at finding quasars in data sets with no u band and in redshift ranges where exclusively photometric selection is not efficient. We show that quasars' rest-frame ensemble variability, measured as a root mean squared in [Delta] magnitudes, is consistent with V(z, L, t) = A sub(0)(1 + z) super(0.37)(L/L sub(0)) super(-0.16)(t/1 yr) super(0.246), where L sub(0) = 10 super(46) erg s super(-1) and A sub(0) = 0.190, 0.162, 0.147, or 0.141 in the g sub(P1), r sub(P1), i sub(P1), or z sub(P1) filter, respectively. We also fit across all four filters and obtain median variability as a function of z, L, and [lambda] as V(z, L, [lambda], t) = 0.079(1 + z) super(0.15)(L/L sub(0)) super(-0.2)([lambda]/1000nm) super(-0.44)(t /1 yr) super(0.246).</description><identifier>ISSN: 0004-637X</identifier><identifier>EISSN: 1538-4357</identifier><identifier>DOI: 10.1088/0004-637X/784/2/92</identifier><language>eng</language><publisher>United States</publisher><subject>ASTROPHYSICS, COSMOLOGY AND ASTRONOMY ; COLOR ; Deltas ; IMPURITIES ; Photometry ; Power law ; QUASARS ; RED SHIFT ; Sky surveys (astronomy) ; SPECTROSCOPY ; TELESCOPES</subject><ispartof>The Astrophysical journal, 2014-04, Vol.784 (2), p.1-16</ispartof><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c385t-fd64614d505ce6963531458bc97e3882681f4bcc0758b7d9859187e486204d803</citedby><cites>FETCH-LOGICAL-c385t-fd64614d505ce6963531458bc97e3882681f4bcc0758b7d9859187e486204d803</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,776,780,881,27901,27902</link.rule.ids><backlink>$$Uhttps://www.osti.gov/biblio/22357288$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Morganson, E</creatorcontrib><creatorcontrib>Burgett, W S</creatorcontrib><creatorcontrib>Chambers, K C</creatorcontrib><creatorcontrib>Green, P J</creatorcontrib><creatorcontrib>Kaiser, N</creatorcontrib><creatorcontrib>Magnier, E A</creatorcontrib><creatorcontrib>Marshall, P J</creatorcontrib><creatorcontrib>Morgan, J S</creatorcontrib><creatorcontrib>Price, P A</creatorcontrib><creatorcontrib>Rix, H-W</creatorcontrib><creatorcontrib>Schlafly, E F</creatorcontrib><creatorcontrib>Tonry, J L</creatorcontrib><creatorcontrib>Walter, F</creatorcontrib><title>MEASURING QUASAR VARIABILITY WITH Pan-STARRS1 AND SDSS</title><title>The Astrophysical journal</title><description>We measure quasar variability using the Panoramic Survey Telescope and Rapid Response System 1 Survey (Pan-STARRS1 or PS1) and the Sloan Digital Sky Survey (SDSS) and establish a method of selecting quasars via their variability in 10 super(4) deg super(2) surveys. We use 10 super(5) spectroscopically confirmed quasars that have been well measured in both PSI and SDSS and take advantage of the decadal timescales that separate SDSS measurements and PS1 measurements. A power law model fits the data well over the entire time range tested, 0.01-10 yr. Variability in the current PS1-SDSS data set can efficiently distinguish between quasars and nonvarying objects. It improves the purity of a griz quasar color cut from 4.1% to 48% while maintaining 67% completeness. Variability will be very effective at finding quasars in data sets with no u band and in redshift ranges where exclusively photometric selection is not efficient. We show that quasars' rest-frame ensemble variability, measured as a root mean squared in [Delta] magnitudes, is consistent with V(z, L, t) = A sub(0)(1 + z) super(0.37)(L/L sub(0)) super(-0.16)(t/1 yr) super(0.246), where L sub(0) = 10 super(46) erg s super(-1) and A sub(0) = 0.190, 0.162, 0.147, or 0.141 in the g sub(P1), r sub(P1), i sub(P1), or z sub(P1) filter, respectively. We also fit across all four filters and obtain median variability as a function of z, L, and [lambda] as V(z, L, [lambda], t) = 0.079(1 + z) super(0.15)(L/L sub(0)) super(-0.2)([lambda]/1000nm) super(-0.44)(t /1 yr) super(0.246).</description><subject>ASTROPHYSICS, COSMOLOGY AND ASTRONOMY</subject><subject>COLOR</subject><subject>Deltas</subject><subject>IMPURITIES</subject><subject>Photometry</subject><subject>Power law</subject><subject>QUASARS</subject><subject>RED SHIFT</subject><subject>Sky surveys (astronomy)</subject><subject>SPECTROSCOPY</subject><subject>TELESCOPES</subject><issn>0004-637X</issn><issn>1538-4357</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2014</creationdate><recordtype>article</recordtype><recordid>eNqNkMtKw0AUhgdRsFZfwFXAjZuYuV-WY61toFZNUi-rIZ1MMNImNZMufHsTKq5dHc7h4_D_HwCXCN4gKGUEIaQhJ-ItEpJGOFL4CIwQIzKkhIljMPoDTsGZ95_DipUaAf4w1ekqiZez4HmlU50ELzqJ9W28iLP34DXO5sFTXodpppMkRYFe3gXpXZqeg5My33h38TvHYHU_zSbzcPE4iyd6EVoiWReWBacc0YJBZh1XnDCCKJNrq4QjUmIuUUnX1kLRH0WhJFNICkclx5AWEpIxuDr8bXxXGW-rztkP29S1s53BuO-Gpeyp6wO1a5uvvfOd2Vbeus0mr12z9wYJAmGfhKt_oAgLrpREPYoPqG0b71tXml1bbfP22yBoButmsGgGqaa3brBRmPwABKFsug</recordid><startdate>20140401</startdate><enddate>20140401</enddate><creator>Morganson, E</creator><creator>Burgett, W S</creator><creator>Chambers, K C</creator><creator>Green, P J</creator><creator>Kaiser, N</creator><creator>Magnier, E A</creator><creator>Marshall, P J</creator><creator>Morgan, J S</creator><creator>Price, P A</creator><creator>Rix, H-W</creator><creator>Schlafly, E F</creator><creator>Tonry, J L</creator><creator>Walter, F</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>20140401</creationdate><title>MEASURING QUASAR VARIABILITY WITH Pan-STARRS1 AND SDSS</title><author>Morganson, E ; Burgett, W S ; Chambers, K C ; Green, P J ; Kaiser, N ; Magnier, E A ; Marshall, P J ; Morgan, J S ; Price, P A ; Rix, H-W ; Schlafly, E F ; Tonry, J L ; Walter, F</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c385t-fd64614d505ce6963531458bc97e3882681f4bcc0758b7d9859187e486204d803</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2014</creationdate><topic>ASTROPHYSICS, COSMOLOGY AND ASTRONOMY</topic><topic>COLOR</topic><topic>Deltas</topic><topic>IMPURITIES</topic><topic>Photometry</topic><topic>Power law</topic><topic>QUASARS</topic><topic>RED SHIFT</topic><topic>Sky surveys (astronomy)</topic><topic>SPECTROSCOPY</topic><topic>TELESCOPES</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Morganson, E</creatorcontrib><creatorcontrib>Burgett, W S</creatorcontrib><creatorcontrib>Chambers, K C</creatorcontrib><creatorcontrib>Green, P J</creatorcontrib><creatorcontrib>Kaiser, N</creatorcontrib><creatorcontrib>Magnier, E A</creatorcontrib><creatorcontrib>Marshall, P J</creatorcontrib><creatorcontrib>Morgan, J S</creatorcontrib><creatorcontrib>Price, P A</creatorcontrib><creatorcontrib>Rix, H-W</creatorcontrib><creatorcontrib>Schlafly, E F</creatorcontrib><creatorcontrib>Tonry, J L</creatorcontrib><creatorcontrib>Walter, F</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>Morganson, E</au><au>Burgett, W S</au><au>Chambers, K C</au><au>Green, P J</au><au>Kaiser, N</au><au>Magnier, E A</au><au>Marshall, P J</au><au>Morgan, J S</au><au>Price, P A</au><au>Rix, H-W</au><au>Schlafly, E F</au><au>Tonry, J L</au><au>Walter, F</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>MEASURING QUASAR VARIABILITY WITH Pan-STARRS1 AND SDSS</atitle><jtitle>The Astrophysical journal</jtitle><date>2014-04-01</date><risdate>2014</risdate><volume>784</volume><issue>2</issue><spage>1</spage><epage>16</epage><pages>1-16</pages><issn>0004-637X</issn><eissn>1538-4357</eissn><abstract>We measure quasar variability using the Panoramic Survey Telescope and Rapid Response System 1 Survey (Pan-STARRS1 or PS1) and the Sloan Digital Sky Survey (SDSS) and establish a method of selecting quasars via their variability in 10 super(4) deg super(2) surveys. We use 10 super(5) spectroscopically confirmed quasars that have been well measured in both PSI and SDSS and take advantage of the decadal timescales that separate SDSS measurements and PS1 measurements. A power law model fits the data well over the entire time range tested, 0.01-10 yr. Variability in the current PS1-SDSS data set can efficiently distinguish between quasars and nonvarying objects. It improves the purity of a griz quasar color cut from 4.1% to 48% while maintaining 67% completeness. Variability will be very effective at finding quasars in data sets with no u band and in redshift ranges where exclusively photometric selection is not efficient. We show that quasars' rest-frame ensemble variability, measured as a root mean squared in [Delta] magnitudes, is consistent with V(z, L, t) = A sub(0)(1 + z) super(0.37)(L/L sub(0)) super(-0.16)(t/1 yr) super(0.246), where L sub(0) = 10 super(46) erg s super(-1) and A sub(0) = 0.190, 0.162, 0.147, or 0.141 in the g sub(P1), r sub(P1), i sub(P1), or z sub(P1) filter, respectively. We also fit across all four filters and obtain median variability as a function of z, L, and [lambda] as V(z, L, [lambda], t) = 0.079(1 + z) super(0.15)(L/L sub(0)) super(-0.2)([lambda]/1000nm) super(-0.44)(t /1 yr) super(0.246).</abstract><cop>United States</cop><doi>10.1088/0004-637X/784/2/92</doi><tpages>16</tpages><oa>free_for_read</oa></addata></record> |
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subjects | ASTROPHYSICS, COSMOLOGY AND ASTRONOMY COLOR Deltas IMPURITIES Photometry Power law QUASARS RED SHIFT Sky surveys (astronomy) SPECTROSCOPY TELESCOPES |
title | MEASURING QUASAR VARIABILITY WITH Pan-STARRS1 AND SDSS |
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