<?xml version="1.0" encoding="ISO-8859-1"?><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance">
<front>
<journal-meta>
<journal-id>0035-001X</journal-id>
<journal-title><![CDATA[Revista mexicana de física]]></journal-title>
<abbrev-journal-title><![CDATA[Rev. mex. fis.]]></abbrev-journal-title>
<issn>0035-001X</issn>
<publisher>
<publisher-name><![CDATA[Sociedad Mexicana de Física]]></publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id>S0035-001X2006000600004</article-id>
<title-group>
<article-title xml:lang="en"><![CDATA[Some statistical mechanical properties of photon black holes]]></article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Hernandez]]></surname>
<given-names><![CDATA[X]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Lopez-Monsalvo]]></surname>
<given-names><![CDATA[C.S]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Mendoza]]></surname>
<given-names><![CDATA[S]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Sussman]]></surname>
<given-names><![CDATA[R.A]]></given-names>
</name>
<xref ref-type="aff" rid="A02"/>
</contrib>
</contrib-group>
<aff id="A01">
<institution><![CDATA[,Universidad Nacional Autónoma de México Instituto de Astronomía ]]></institution>
<addr-line><![CDATA[ Distrito Federal]]></addr-line>
<country>México</country>
</aff>
<aff id="A02">
<institution><![CDATA[,Universidad Nacional Autónoma de México Instituto de Ciencias Nucleares ]]></institution>
<addr-line><![CDATA[ Distrito Federal]]></addr-line>
<country>México</country>
</aff>
<pub-date pub-type="pub">
<day>00</day>
<month>12</month>
<year>2006</year>
</pub-date>
<pub-date pub-type="epub">
<day>00</day>
<month>12</month>
<year>2006</year>
</pub-date>
<volume>52</volume>
<numero>6</numero>
<fpage>515</fpage>
<lpage>521</lpage>
<copyright-statement/>
<copyright-year/>
<self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_arttext&amp;pid=S0035-001X2006000600004&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_abstract&amp;pid=S0035-001X2006000600004&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_pdf&amp;pid=S0035-001X2006000600004&amp;lng=en&amp;nrm=iso"></self-uri><abstract abstract-type="short" xml:lang="en"><p><![CDATA[We show that if the total internal energy of a blackhole is constructed as the sum of N photons all having a fixed wavelength chosento scale with the Schwarzschild radius as &#955; = &#945;Rs, then N will scale with<img border=0 src="../../../../../img/revistas/rmf/v52n6/a4s1.jpg">. A statistical mechanical calculation of the configuration proposed yields &#945; = 4&#960;²/ ln(2) and a total entropy of the system S = kB N ln(2), in agreement with the Bekenstein entropy of a black hole. It is shown that the critical temperature for Bose-Einstein condensation for relativistic particles of &#955; = &#945;Rs is always well below the Hawking temperature of a black hole, in support of the proposed internal configuration. We then examine our results from the point of view of recent loop quantum gravity ideas and find that a natural consistency of both approaches appears. We show that the Jeans criterion for gravitational instability can be generalised to the special and general relativistic regimes and holds for any type of mass-energy distribution.]]></p></abstract>
<abstract abstract-type="short" xml:lang="es"><p><![CDATA[En este artículo estudiamos la relación entre la energía y la entropía de un gas de fotones tipo cuerpo negro, contenido dentro de un recinto adiabatico de radio R , cuando es comprimido hacia un régimen auto-gravitacional. Mostramos que este régimen coincide aproximadamente con el régimen de un agujero negro para el sistema, i.e., R &#732;Rs donde Rs representa al radio de Schwarzschild del sistema. La entropía del sistema resulta estar siempre por debajo de la cota Holografíca, incluso cuando R <img border=0 src="../../../../../img/revistas/rmf/v52n6/a4s2.jpg">Rs. Una posible configuración cuántica para el gas de fotones a R <img border=0 src="../../../../../img/revistas/rmf/v52n6/a4s2.jpg">Rs se sugiere, la cual satisface todas las condiciones de agujero negro para la energía, entropía y temperatura. Finalmente, examinamos nuestros resultados desde el punto de vista de algunas ideas recientes de Loop Quantum Gravity.]]></p></abstract>
<kwd-group>
<kwd lng="en"><![CDATA[Physics of black holes]]></kwd>
<kwd lng="en"><![CDATA[classical black holes]]></kwd>
<kwd lng="en"><![CDATA[quantum aspects of black holes]]></kwd>
<kwd lng="en"><![CDATA[evaporation]]></kwd>
<kwd lng="en"><![CDATA[thermodynamics]]></kwd>
<kwd lng="es"><![CDATA[Física de agujeros negros]]></kwd>
<kwd lng="es"><![CDATA[agujeros negros classicos]]></kwd>
<kwd lng="es"><![CDATA[aspectos cuánticos de agujeros negros]]></kwd>
<kwd lng="es"><![CDATA[evaporación]]></kwd>
<kwd lng="es"><![CDATA[termodinámica]]></kwd>
</kwd-group>
</article-meta>
</front><body><![CDATA[ <p align="justify"><font face="verdana" size="4">Investigaci&oacute;n</font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="center"><font face="verdana" size="4"><b>Some statistical mechanical properties of photon black holes</b></font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="center"><font face="verdana" size="2"><b> X. Hernandez,&ordf; C.S. Lopez-Monsalvo&ordf;, S. Mendoza&ordf; and R.A. Sussman<sup>b</sup></b></font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2"><i>&ordf; Instituto de Astronom&iacute;a, Universidad Nacional Aut&oacute;noma de M&eacute;xico, Apartado Postal 70-264, Distrito Federal 04510, M&eacute;xico,    <br> e-mail: <a href="mailto:xavier@astroscu.unam.mx">xavier@astroscu.unam.mx</a> , <a href="mailto:cslopez@astroscu.unam.mx">cslopez@astroscu.unam.mx</a> , <a href="mailto:sergio@astroscu.unam.mx">sergio@astroscu.unam.mx</a></i></font></p>     <p align="justify"><font face="verdana" size="2"><i><sup>b </sup>Instituto de Ciencias Nucleares, Universidad Nacional Aut&oacute;noma de M&eacute;xico, Apartado Postal 70-543, Distrito Federal 04510, M&eacute;xico, e-mail: <a href="mailto:sussman@nuclecu.unam.mx">sussman@nuclecu.unam.mx</a></i></font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     ]]></body>
<body><![CDATA[<p align="justify"><font face="verdana" size="2">Recibido el 3 de noviembre de 06    <br>   Aceptado el 17 de noviembre de 06</font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2"><b>Abstract</b></font></p>     <p align="justify"><font face="verdana" size="2">We show that if the total internal energy of a blackhole is constructed as the sum of N photons all having a fixed wavelength chosento scale with the Schwarzschild radius as  &lambda; = &alpha;<i>R<sub>s</sub>, </i>then <i>N</i> will scale with<img src="/img/revistas/rmf/v52n6/a4s1.jpg">. A statistical mechanical calculation of the configuration proposed yields &alpha; = 4&pi;<sup>2</sup>/ ln(2) and a total entropy of the system <i>S </i>= k<i><sub>B</sub></i><i>N </i> ln(2), in agreement with the Bekenstein entropy of a black hole. It is shown that the critical temperature for Bose-Einstein condensation for relativistic particles of   &lambda; = &alpha;<i>R<sub>s</sub> </i>is always well below the Hawking temperature of a black hole, in support of the proposed internal configuration. We then examine our results from the point of view of recent loop quantum gravity ideas and find that a natural consistency of both approaches appears. We show that the Jeans criterion for gravitational instability can be generalised to the special and general relativistic regimes and holds for any type of mass-energy distribution.</font></p>     <p align="justify"><font face="verdana" size="2"><b>Keywords: </b>Physics of black holes; classical black holes; quantum aspects of black holes; evaporation; thermodynamics.</font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2"><b>Resumen</b></font></p>     <p align="justify"><font face="verdana" size="2">En este art&iacute;culo estudiamos la relaci&oacute;n entre la energ&iacute;a y la entrop&iacute;a de un gas de fotones tipo cuerpo negro, contenido dentro de un recinto adiabatico de radio <i>R , </i>cuando es comprimido hacia un r&eacute;gimen auto-gravitacional. Mostramos que este r&eacute;gimen coincide aproximadamente con el r&eacute;gimen de un agujero negro para el sistema, <i>i.e., R </i> &tilde;<i>R<sub>s </sub></i>donde <i>R<sub>s</sub> </i>representa al radio de Schwarzschild del sistema. La entrop&iacute;a del sistema resulta estar siempre por debajo de la cota Holograf&iacute;ca, incluso cuando <i>R </i><img src="/img/revistas/rmf/v52n6/a4s2.jpg"><i>R<sub>s</sub>. </i>Una posible configuraci&oacute;n cu&aacute;ntica para el gas de fotones a <i>R </i><img src="/img/revistas/rmf/v52n6/a4s2.jpg"><i>R<sub>s</sub> </i>se sugiere, la cual satisface todas las condiciones de agujero negro para la energ&iacute;a, entrop&iacute;a y temperatura. Finalmente, examinamos nuestros resultados desde el punto de vista de algunas ideas recientes de Loop Quantum Gravity.</font></p>     <p align="justify"><font face="verdana" size="2"><b>Descriptores: </b>F&iacute;sica de agujeros negros; agujeros negros classicos; aspectos cu&aacute;nticos de agujeros negros; evaporaci&oacute;n; termodin&aacute;mica.</font></p>     ]]></body>
<body><![CDATA[<p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2">PACS: 04.70.-s; 04.70.Bw; 04.70.Dy</font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2"><a href="/pdf/rmf/v52n6/v52n6a4.pdf">DESCARGAR ART&Iacute;CULO EN FORMATO PDF</a></font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2"><b>Acknowledgements</b></font></p>     <p align="justify"><font face="verdana" size="2">X. Hernandez acknowledges the support of grant UNAM DGAPA (IN117803-3), CONACyT (42809/A-1) and CONACyT (42748). C. Lopez-Monsalvo is grateful for economic support from UNAM DGAPA (IN119203). S. Mendoza gratefully acknowledges financial support from CONACyT (41443) and UNAM DGAPA (IN119203).   We thank the anonymous referee for his comments and suggestions, which improved the final version of the paper.</font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2"><b>References</b></font></p>     <!-- ref --><p align="justify"><font face="verdana" size="2">1. S. Chandrasekhar, <i>The Mathematical Theory of Black Holes, </i>Oxford Classic Texts in the Physical Sciences (Oxford University Press, 2000).</font>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8321664&pid=S0035-001X200600060000400001&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --><!-- ref --><p align="justify"><font face="verdana" size="2">2. V.P Frolov &amp; I.D. 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