<?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>0185-1101</journal-id>
<journal-title><![CDATA[Revista mexicana de astronomía y astrofísica]]></journal-title>
<abbrev-journal-title><![CDATA[Rev. mex. astron. astrofis]]></abbrev-journal-title>
<issn>0185-1101</issn>
<publisher>
<publisher-name><![CDATA[Universidad Nacional Autónoma de México, Instituto de Astronomía]]></publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id>S0185-11012008000100011</article-id>
<title-group>
<article-title xml:lang="en"><![CDATA[Flat central density profiles from scalar field dark matter halos]]></article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Bernal]]></surname>
<given-names><![CDATA[Argelia]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Matos]]></surname>
<given-names><![CDATA[Tonatiuh]]></given-names>
</name>
<xref ref-type="aff" rid="A03"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Núñez]]></surname>
<given-names><![CDATA[Darío]]></given-names>
</name>
<xref ref-type="aff" rid="A02"/>
</contrib>
</contrib-group>
<aff id="A01">
<institution><![CDATA[,Instituto Politécnico Nacional Centro de Investigación y de Estudios Avanzados Departamento de Física]]></institution>
<addr-line><![CDATA[D. F. ]]></addr-line>
<country>México</country>
</aff>
<aff id="A02">
<institution><![CDATA[,Universidad Nacional Autónoma de México Instituto de Ciencias Nucleares ]]></institution>
<addr-line><![CDATA[D. F. ]]></addr-line>
<country>México</country>
</aff>
<aff id="A03">
<institution><![CDATA[,Instituto Avanzado de Cosmología (IAC)  ]]></institution>
<addr-line><![CDATA[ ]]></addr-line>
<country>México</country>
</aff>
<pub-date pub-type="pub">
<day>00</day>
<month>00</month>
<year>2008</year>
</pub-date>
<pub-date pub-type="epub">
<day>00</day>
<month>00</month>
<year>2008</year>
</pub-date>
<volume>44</volume>
<numero>1</numero>
<fpage>149</fpage>
<lpage>160</lpage>
<copyright-statement/>
<copyright-year/>
<self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_arttext&amp;pid=S0185-11012008000100011&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_abstract&amp;pid=S0185-11012008000100011&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_pdf&amp;pid=S0185-11012008000100011&amp;lng=en&amp;nrm=iso"></self-uri><abstract abstract-type="short" xml:lang="es"><p><![CDATA[El campo escalar con un potencial cosh se comporta en el régimen lineal justo como la materia oscura fría (CDM). Así, la hipótesis de materia oscura escalar (SFDM) predice la misma formación de estructura que CDM. Los parámetros libres del modelo SFDM se fijan con observaciones cosmológicas. En un trabajo anterior mostramos que con dichos valores, la SFDM se colapsa y forma objetos estables con masa del orden de 10(12)M<img border=0 src="../../../../../img/revistas/rmaa/v44n1/a11s1.jpg">. En este trabajo utilizamos soluciones analíticas para las ecuaciones de Einstein-Klein-Gordon en el caso plano y en el límite de campo débil y mostramos que el perfil de densidad de SFDM corresponde al de una densidad central casi plana y que coincide con el del modelo de CDM en una amplia zona de la región exterior. Este resultado podría resolver el problema de los picos de densidad de CDM sin ninguna hipótesis adicional, lo que apoya la viabilidad del modelo de SFDM.]]></p></abstract>
<abstract abstract-type="short" xml:lang="en"><p><![CDATA[Scalar fields endowed with a cosh potential behave in the linear regime, exactly as the cold dark matter (CDM) model. Thus, the scalar field dark matter (SFDM) hypothesis predicts the same structure formation as the CDM model. This means that CDM and SFDM are equivalent from the cosmological point of view. The free parameters of the SFDM model are determined by cosmological observations. In previous work we showed that if we use such parameters, the scalar field collapses forming stable objects with a mass around 10(12)M<img border=0 width=32 height=32 src="../../../../../img/revistas/rmaa/v44n1/a11s1.jpg">. In the present work we use analytical solutions of the flat and weak field limit of the Einstein-Klein-Gordon equations and show that the SFDM density profile corresponds to a halo with an almost flat central density and that it coincides with the CDM model in a broad outer region. This result could solve the problem of the density cusp DM halo in galaxies without any additional hypothesis, thus supporting the viability of the SFDM model.]]></p></abstract>
<kwd-group>
<kwd lng="en"><![CDATA[dark matter]]></kwd>
<kwd lng="en"><![CDATA[galaxies: formation]]></kwd>
<kwd lng="en"><![CDATA[galaxies: halos]]></kwd>
</kwd-group>
</article-meta>
</front><body><![CDATA[ <p align="center"><font face="verdana" size="4"><b>Flat central density profiles from scalar field dark matter halos</b></font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="center"><font face="verdana" size="2"><b>Argelia Bernal,<sup>1,3</sup> Tonatiuh Matos,<sup>1,3</sup> and Dar&iacute;o N&uacute;&ntilde;ez <sup>2,3</sup></b></font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2">1 <i>Departamento de F&iacute;sica, Centro de Investigaci&oacute;n y de Estudios Avanzados del IPN, Apdo. Postal 14&#150;740, 07000 M&eacute;xico, D. F., M&eacute;xico <a href="http://www.fis.cinvestav.mx/%7Etmatos/" target="_blank">http://www.fis.cinvestav.mx/~tmatos</a> (<a href="mailto:abernal@fis.cinvestav.mx">abernal@fis.cinvestav.mx</a>, <a href="mailto:tmatos@fis.cinvestav.mx">tmatos@fis.cinvestav.mx</a>)</i></font></p>     <p align="justify"><font face="verdana" size="2"><sup>2</sup> <i>Instituto de Ciencias Nucleares, Universidad Nacional Aut&oacute;noma de M&eacute;xico, Apdo. Postal 70&#150;543, 04510 M&eacute;xico, D. F., M&eacute;xico. On Sabbathicak leave at Max&#150;Planck&#150;Institut f&uuml;r Gravitationsphysik, Albert Einstein Institut, 14476 Golm, Germany (<a href="mailto:nunez@nuclecu.unam.mx">nunez@nuclecu.unam.mx</a>)</i></font></p>     <p align="justify"><font face="verdana" size="2"><sup>3</sup> <i>Part of the Instituto Avanzado de Cosmolog&iacute;a (IAC), M&eacute;xico.</i></font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2">Received 2006 May 24    <br>   Accepted 2008 January 10</font></p>     ]]></body>
<body><![CDATA[<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">El campo escalar con un potencial cosh se comporta en el r&eacute;gimen lineal justo como la materia oscura fr&iacute;a (CDM). As&iacute;, la hip&oacute;tesis de materia oscura escalar (SFDM) predice la misma formaci&oacute;n de estructura que CDM. Los par&aacute;metros libres del modelo SFDM se fijan con observaciones cosmol&oacute;gicas. En un trabajo anterior mostramos que con dichos valores, la SFDM se colapsa y forma objetos estables con masa del orden de 10<sup>12</sup><i>M</i><sub><img src="/img/revistas/rmaa/v44n1/a11s1.jpg"></sub>. En este trabajo utilizamos soluciones anal&iacute;ticas para las ecuaciones de Einstein&#150;Klein&#150;Gordon en el caso plano y en el l&iacute;mite de campo d&eacute;bil y mostramos que el perfil de densidad de SFDM corresponde al de una densidad central casi plana y que coincide con el del modelo de CDM en una amplia zona de la regi&oacute;n exterior. Este resultado podr&iacute;a resolver el problema de los picos de densidad de CDM sin ninguna hip&oacute;tesis adicional, lo que apoya la viabilidad del modelo de SFDM.</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">Scalar fields endowed with a cosh potential behave in the linear regime, exactly as the cold dark matter (CDM) model. Thus, the scalar field dark matter (SFDM) hypothesis predicts the same structure formation as the CDM model. This means that CDM and SFDM are equivalent from the cosmological point of view. The free parameters of the SFDM model are determined by cosmological observations. In previous work we showed that if we use such parameters, the scalar field collapses forming stable objects with a mass around 10<sup>12</sup><i>M</i><sub><sub><img src="/img/revistas/rmaa/v44n1/a11s1.jpg"></sub></sub>. In the present work we use analytical solutions of the flat and weak field limit of the Einstein&#150;Klein&#150;Gordon equations and show that the SFDM density profile corresponds to a halo with an almost flat central density and that it coincides with the CDM model in a broad outer region. This result could solve the problem of the density cusp DM halo in galaxies without any additional hypothesis, thus supporting the viability of the SFDM model.</font></p>     <p align="justify"><font face="verdana" size="2"><i><b>Key Words: </b></i>dark matter &#151; galaxies: formation &#151; galaxies: halos</font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2"><a href="/pdf/rmaa/v44n1/v44n1a11.pdf">DESCARGAR ART&Iacute;CULO EN FOMATO PDF </a></font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     ]]></body>
<body><![CDATA[<p align="justify"><font face="verdana" size="2"><b>Acknowledgements</b></font></p>     <p align="justify"><font face="verdana" size="2">We would like to thank Miguel Alcubierre, Vladimir &Aacute;vila Reese, Arturo Ure&ntilde;a and F. Siddhartha Guzm&aacute;n for many helpful and useful discussions, and Erasmo G&oacute;mez and Aurelio Esp&iacute;ritu for technical support. We thank Lidia Rojas for carefull reading and suggestions to improve our work. The numeric computations were carried out in the "Laboratorio de S&uacute;per&#150;C&oacute;mputo Astrof&iacute;sico (LaSumA) del Cinvestav". This work was partly supported by Conacyt M&eacute;xico, under grants 32138&#150;E,47209&#150;F and 42748 and by grant number I0101/131/07 C&#150;234/07, Instituto Avanzado de Cosmolog&iacute;a (IAC) collaboration. Also by the bilateral Mexican&#150;German project DFG&#150;Conacyt 444 MEX&#150;13/17/0&#150;1.</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">Alcubierre, M., Becerril, R., Guzm&aacute;n, F. S., Matos, T., N&uacute;&ntilde;ez,   D., &amp; Ure&ntilde;a&#150;L&oacute;pez,   L.  A.   2003,   Classical Quantum Gravity, 20, 2883</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=7422935&pid=S0185-1101200800010001100001&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">Alcubierre, M., Guzm&aacute;n, F. S., Matos, T., N&uacute;&ntilde;ez, D., Ure&ntilde;a&#150;L&oacute;pez, L. 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