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    <pubDate>Wed, 22 May 2013 04:07:29 GMT</pubDate>
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      <title>The bolometric luminosity of type 2 AGN from extinction-corrected [OIII]: no evidence of Eddington-limited sources</title>
      <link>http://hdl.handle.net/2307/391</link>
      <description>&lt;Title&gt;The bolometric luminosity of type 2 AGN from extinction-corrected [OIII]: no evidence of Eddington-limited sources&lt;/Title&gt;
&lt;Authors&gt;Lamastra, Alessandra; Bianchi, Stefano; Matt, Giorgio; Perola, Giuseppe Cesare; Barcons, X.; Carrera, F. J.&lt;/Authors&gt;
&lt;Issue Date&gt;2009-09&lt;/Issue Date&gt;
&lt;Is part of&gt;Astronomy &amp; Astrophysics&lt;/Is part of&gt;
&lt;Volume&gt;504&lt;/Volume&gt;
&lt;Pages&gt;73-79&lt;/Pages&gt;
&lt;Abstract&gt;Context. There have been recent claims that a significant fraction of type 2 AGN accrete close to or even above the Eddington limit. In type 2 AGN, the bolometric luminosity (L-b) is generally inferred from the [OIII] emission line luminosity (L-OIII). The key issue in estimating the bolometric luminosity in these AGN, is therefore to know the bolometric correction to be applied to L-OIII. A complication arises from the observed L-OIII being affected by extinction, most likely from dust within the narrow line region. The extinction-corrected [OIII] luminosity (L-OIII(c)) is a better estimator of the nuclear luminosity than L-OIII. However, only the bolometric correction to be applied to the uncorrected L-OIII has been evaluated so far. Aims. This paper is devoted to estimating the bolometric correction C-OIII = L-b/L-OIII(c) for deriving the Eddington ratios for the type 2 AGN in a sample of SDSS objects. Methods. We collected 61 sources from the literature with reliable estimates of both L-OIII(c) and X-ray luminosities (L-X). To estimate C-OIII, we combined the observed correlation between L-OIII(c) and L-Xwith the X-ray bolometric correction. Results. In contrast to previous studies, we found a linear correlation between L-OIII(c) and L-X. We estimated C-OIII using an earlier luminosity-dependent X-ray bolometric correction, and we found a mean value of C-OIII in the luminosity ranges log L-OIII = 38-40, 40-42, and 42-44 of 87, 142, and 454, respectively. We used it to calculate the Eddington ratio distribution of type 2 SDSS AGN at 0.3 &lt; z &lt; 0.4 and found that these sources are not accreting near their Eddington limit, contrary to previous claims.&lt;/Abstract&gt;</description>
      <pubDate>Mon, 31 Aug 2009 22:00:00 GMT</pubDate>
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      <dc:date>2009-08-31T22:00:00Z</dc:date>
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