<?xml version="1.0" encoding="UTF-8"?>
<!DOCTYPE dataset SYSTEM "http://tarantella.gsfc.nasa.gov/xml/dataset_048.dtd">
<dataset subject="astronomy" xmlns:xlink="http://www.w3.org/XML/XLink/0.9">
	<title>A study of quasar absorption-line systems with IRAS</title>
	<altname type="ADC">J/AJ/112/62</altname>
		<altname type="CDS">J/AJ/112/62</altname>
		<altname type="brief">Quasar absorption-line systems</altname>
	<reference>
		<source>
<journal>
	<title>A study of quasar absorption-line systems with IRAS</title>
	<author>
			<initial>A</initial>
			<initial>M</initial>
			<lastName>Tanner</lastName></author>
	<author>
			<initial>J</initial>
			<lastName>Bechtold</lastName></author>
	<author>
			<initial>C</initial>
			<initial>E</initial>
			<lastName>Walker</lastName></author>
	<author>
			<initial>J</initial>
			<initial>H</initial>
			<lastName>Black</lastName></author>
	<author>
			<initial>R</initial>
			<initial>M</initial>
			<lastName>Cutri</lastName></author>
	<name>Astron. J.</name>
	<volume>112</volume>
	<pageno>62</pageno>
		<date>
			<year>1996</year></date>
	<bibcode>1996AJ....112...62T</bibcode></journal></source></reference>
	<keywords parentListURL="http://messier.gsfc.nasa.gov/xml/keywordlists/adc_keywords.html">
			<keyword xlink:href="Photometry_infrared.html">Photometry, infrared</keyword>
			<keyword xlink:href="QSOs.html">QSOs</keyword>
			<keyword xlink:href="Redshifts.html">Redshifts</keyword></keywords>
	<descriptions>
				<abstract>
					<para>
    A survey of quasar absorbers was conducted using the Infrared
    Astronomical Satellite (IRAS) database. Quasars with known intervening
    absorption-line systems and broad absorption line (BAL) QSOs were
    selected primarily from Junkkarinen et al. (1991ApJS...77..203J). Of
    the 570 quasars with IRAS data, 52 showed 3{sigma} or better
    detections in at least one band in SCANPI analysis. The origin of the
    IRAS flux could be from the absorption-line systems, other galaxies,
    or the quasar itself. The spectral energy distributions for quasars
    detected in the absorption-line sample and BAL QSOs were found to be
    redder than those of two control samples which suggests that some of
    the IRAS flux may arise in dust associated with the intervening
    galaxies. IRAS SUPERSCANPI processing was carried out for 77 quasars
    with known Mg II absorption at Zabs&lt;1 to investigate the ensemble
    far-infrared properties of these objects. SUPERSCANPI processing
    evaluates the median flux for many different positions on the sky,
    resulting in an improvement in the effective sensitivity. A control
    sample consisting of objects with no Mg II absorption known at Zabs&lt;1
    but with the same distribution of absolute V-magnitude, Zem and
    radio-loud fraction for the background quasars was also processed. The
    Mg II sample was detected at 3{sigma} or better in all four IRAS bands
    with a significantly larger flux than the control sample at 60{mu}m
    and 100{mu}m. If this far-infrared emission is from the absorber
    galaxies, then the far-infrared luminosity of the composite Mg II
    absorber was found to be comparable to that of a starbursting galaxy,
    although such a high star-formation rate is inconsistent with the
    optical and near-infrared colors of low-redshift Mg II systems. Four
    of the quasars with individual IRAS detections have intervening
    galaxies identified with the Mg II absorption-lines. The spectral
    energy distributions of these galaxies imply far-infrared luminosities
    in excess of what Arp 220 would give at their redshifts. While all the
    external evidence suggests that the detection of far-infrared emission
    from the absorber sample may not be connected to the presence of the
    Mg II absorber, we discuss future observations which may help explain
    our results.</para></abstract>
                        <details><para><observatory base="space"> IRAS</observatory></para></details></descriptions>
	<tableHead>
		<tableLinks>
				<tableLink xlink:href="table1">
	<title>Additional quasar in absorption-line (AL) sample,
                               not in JHB (Cat. &lt;J/ApJS/77/203>)</title></tableLink>
				<tableLink xlink:href="table2">
	<title>Damped Ly{alpha} sample</title></tableLink></tableLinks>
	<fields>
		<field>
			<name>QSO</name>
			<definition>Quasar name</definition>
			<units>---</units></field>
		<field>
			<name>r_QSO</name>
			<definition>Reference
	<footnote footnoteId="???"><para>number=1</para>
			<para>a : Steidel &amp; Sargent (1992ApJS...80....1S)
          b : Aldcroft et al. (1994ApJS...93....1A)
          c : Lanzetta et al. (1991ApJS...77....1L)
          d : Junkkarinen et al. (1991, Cat. &lt;J/ApJS/77/203>)
          e : White et al. (1993ApJ...407..456W)
          f : Turnshek et al. (1989ApJ...344..567T)
          g : Wolfe et al. (1986ApJS...61..249W)
          h : Francis &amp; Hewitt (1993AJ....105.1633F)</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>zem</name>
			<definition>Emission redshift</definition>
			<units>---</units></field>
		<field>
			<name>zabs</name>
			<definition>Absorption redshift</definition>
			<units>---</units></field>
		<field>
			<name>Vmag</name>
			<definition>V magnitude from Hewitt &amp; Burbidge
                                     (1993ApJS...87..451H)</definition>
			<units>mag</units></field>
		<field>
			<name>RL</name>
			<definition>Radio loudness
	<footnote footnoteId="???"><para>number=2</para>
			<para>RL=log[f_v_(5GHz)/f_v_(V)], where f_v_(5GHz) is the radio flux density
              at 5GHz and [f_v_(V) is the V band flux density, based on 5 GHz
              flux densities from Veron-Cetty &amp; Veron (1987, See Cat. VII/188)
</para></footnote></definition>
			<units>---</units></field></fields></tableHead>
	<tableHead>
		<tableLinks>
				<tableLink xlink:href="table3">
	<title>IRAS ADDSCAN detections</title></tableLink>
				<tableLink xlink:href="table4">
	<title>BAL QSO's detected with IRAS ADDSCAN analysis</title></tableLink></tableLinks>
	<fields>
		<field>
			<name>QSO</name>
			<definition>Quasar name</definition>
			<units>---</units></field>
		<field>
			<name>Note</name>
			<definition>Note
	<footnote footnoteId="???"><para>number=1</para>
			<para>c : galaxies or quasars in vicinity visible on Palomar Sky Survey.
          d : UGC 439, IRAS source is 45 arcseconds northwest of quasar.
          e : bright stars nearby visible on Palomar Sky Survey.
          f : IRAS source is 1 arcminute northwest of quasar.
          g : IRAS source is 30 arcseconds southeast of quasar.
          h : IRAS source is 1 arcminute north of quasar.
          i : NGC 3067, IRAS source is 2 arcminutes southwest of quasar.
          k : IRAS source is 1 arcminute south of quasar.
          l : NGC 6045.
          m : ESO 400-G012.</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>zem</name>
			<definition>Emission redshift</definition>
			<units>---</units></field>
		<field>
			<name>Vmag</name>
			<definition>V magnitude</definition>
			<units>mag</units></field>
		<field>
			<name>zabs</name>
			<definition>Absorption redshift</definition>
			<units>---</units></field>
		<field>
			<name>RAh</name>
			<definition>Right ascension (1950.0)</definition>
			<units>h</units></field>
		<field>
			<name>RAm</name>
			<definition>Right ascension (1950.0)</definition>
			<units>min</units></field>
		<field>
			<name>RAs</name>
			<definition>Right ascension (1950.0)</definition>
			<units>s</units></field>
		<field>
			<name>DE-</name>
			<definition>Declination</definition>
			<units>---</units></field>
		<field>
			<name>DEd</name>
			<definition>Declination (1950.0)</definition>
			<units>deg</units></field>
		<field>
			<name>DEm</name>
			<definition>Declination (1950.0)</definition>
			<units>arcmin</units></field>
		<field>
			<name>DEs</name>
			<definition>Declination (1950.0)</definition>
			<units>arcsec</units></field>
		<field>
			<name>l_S12um</name>
			<definition>Limit flag on 12um</definition>
			<units>---</units></field>
		<field>
			<name>S12um</name>
			<definition>IRAS flux at 12um
	<footnote footnoteId="???"><para>number=2</para>
			<para>3 sigma upper limits given when not detected</para></footnote></definition>
			<units>Jy</units></field>
		<field>
			<name>e_S12um</name>
			<definition>rms uncertainty on S12um</definition>
			<units>Jy</units></field>
		<field>
			<name>l_S25um</name>
			<definition>Limit flag on 25um</definition>
			<units>---</units></field>
		<field>
			<name>S25um</name>
			<definition>IRAS flux at 25um
	<footnote footnoteId="???"><para>number=2</para>
			<para>3 sigma upper limits given when not detected</para></footnote></definition>
			<units>Jy</units></field>
		<field>
			<name>e_S25um</name>
			<definition>rms uncertainty on S25um</definition>
			<units>Jy</units></field>
		<field>
			<name>l_S60um</name>
			<definition>Limit flag on 60um
	<footnote footnoteId="???"><para>number=2</para>
			<para>3 sigma upper limits given when not detected</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>S60um</name>
			<definition>IRAS flux at 60um</definition>
			<units>Jy</units></field>
		<field>
			<name>e_S60um</name>
			<definition>rms uncertainty on S60um</definition>
			<units>Jy</units></field>
		<field>
			<name>l_S100um</name>
			<definition>Limit flag on 100um
	<footnote footnoteId="???"><para>number=2</para>
			<para>3 sigma upper limits given when not detected</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>S100um</name>
			<definition>IRAS flux at 100um</definition>
			<units>Jy</units></field>
		<field>
			<name>e_S100um</name>
			<definition>rms uncertainty on S100um</definition>
			<units>Jy</units></field>
		<field>
			<name>RL</name>
			<definition>Radio loudness
	<footnote footnoteId="???"><para>number=3</para>
			<para>RL=log[f_v_(5GHz)/f_v_(V)], where f_v_(5GHz) is the radio flux density
              at 5GHz and [f_v_(V) is the V band flux density, based on 5 GHz
              flux densities from Veron-Cetty &amp; Veron (1987, See Cat. VII/188)
              unless otherwise stated.
          j : RL based on 5 GHz flux densities from Kellerman et al.
               (1994AJ....108.1163K).
          B : BL Lac
          O : OVV
</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>n_RL</name>
			<definition>Note on RL
	<footnote footnoteId="???"><para>number=3</para>
			<para>RL=log[f_v_(5GHz)/f_v_(V)], where f_v_(5GHz) is the radio flux density
              at 5GHz and [f_v_(V) is the V band flux density, based on 5 GHz
              flux densities from Veron-Cetty &amp; Veron (1987, See Cat. VII/188)
              unless otherwise stated.
          j : RL based on 5 GHz flux densities from Kellerman et al.
               (1994AJ....108.1163K).
          B : BL Lac
          O : OVV
</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>zabs2</name>
			<definition>Second absorption redshift</definition>
			<units>---</units></field>
		<field>
			<name>zabs3</name>
			<definition>Second absorption redshift</definition>
			<units>---</units></field>
		<field>
			<name>zabs4</name>
			<definition>Second absorption redshift</definition>
			<units>---</units></field>
		<field>
			<name>zabs5</name>
			<definition>Second absorption redshift</definition>
			<units>---</units></field>
		<field>
			<name>zabs6</name>
			<definition>Second absorption redshift</definition>
			<units>---</units></field>
		<field>
			<name>zabs7</name>
			<definition>Second absorption redshift</definition>
			<units>---</units></field>
		<field>
			<name>zabs8</name>
			<definition>Second absorption redshift</definition>
			<units>---</units></field>
		<field>
			<name>zabs9</name>
			<definition>Second absorption redshift</definition>
			<units>---</units></field>
		<field>
			<name>zabs10</name>
			<definition>Second absorption redshift</definition>
			<units>---</units></field></fields></tableHead>
	<tableHead>
		<tableLinks>
				<tableLink xlink:href="table5">
	<title>Low redshift Mg II absorption line sample</title></tableLink>
				<tableLink xlink:href="table6">
	<title>Control sample with no Mg II absorption for Zabs&lt;1</title></tableLink></tableLinks>
	<fields>
		<field>
			<name>QSO</name>
			<definition>Quasar name</definition>
			<units>---</units></field>
		<field>
			<name>n_QSO</name>
			<definition>Note
	<footnote footnoteId="???"><para>number=1</para>
			<para>a: Objects with individual IRAS detections
          b: Removed for the control list for SUPERSCANPI without
              IRAS detections</para></footnote></definition>
			<units>---</units></field>
		<field>
			<name>zem</name>
			<definition>Emission redshift</definition>
			<units>---</units></field>
		<field>
			<name>zabs</name>
			<definition>Absorption redshift</definition>
			<units>---</units></field>
		<field>
			<name>Vmag</name>
			<definition>V magnitude</definition>
			<units>mag</units></field>
		<field>
			<name>RL</name>
			<definition>Radio loudness</definition>
			<units>---</units></field>
		<field>
			<name>Ref</name>
			<definition>References, for table6 only
	<footnote footnoteId="???"><para>number=2</para>
			<para>1: Aldcroft et al. (1994ApJS...93....1A)
          2: Steidel &amp; Sargent (1992ApJS...80....1S)
          3: Barthel et al. (1990A&amp;AS...82..339B)
</para></footnote></definition>
			<units>---</units></field></fields></tableHead>
	
	<history>
		<ingest>
	
			<creator>
				<lastName>James Marcout, Patricia Bauer</lastName>
				<affiliation>CDS</affiliation></creator>
	<date>
		<year>1997</year><month>Jun</month><day>17</day></date></ingest>
		
		<revisions>
	<revision>
		<creator>
			<lastName>UNKNOWN</lastName></creator>
		<date><year>UNKNOWN</year></date>
		<para> Prepared via OCR at CDS.
         In table6, for QSO 0736-0620, V=718.5 in the printed version,
          we change this value in 18.5 in the electronic table</para></revision></revisions></history>
	<identifier>J_AJ_112_62.xml</identifier></dataset>
