<?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>0034-7426</journal-id>
<journal-title><![CDATA[Revista Colombiana de Matemáticas]]></journal-title>
<abbrev-journal-title><![CDATA[Rev.colomb.mat.]]></abbrev-journal-title>
<issn>0034-7426</issn>
<publisher>
<publisher-name><![CDATA[Universidad Nacional de Colombia y Sociedad Colombiana de Matemáticas]]></publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id>S0034-74262008000200006</article-id>
<title-group>
<article-title xml:lang="en"><![CDATA[Chandrasekhar ansatz and the generalized total angular momentum operator for the Dirac equation in the Kerr-Newman metric]]></article-title>
<article-title xml:lang="es"><![CDATA[El ansatz de Chandrasekhar y el operador generalizado del momento angular para la ecuación de Dirac en la métrica de Kerr-Newman]]></article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname><![CDATA[BATIC]]></surname>
<given-names><![CDATA[DAVIDE]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[SCHMID]]></surname>
<given-names><![CDATA[HARALD]]></given-names>
</name>
<xref ref-type="aff" rid="A02"/>
</contrib>
</contrib-group>
<aff id="A01">
<institution><![CDATA[,Universidad de Los Andes  ]]></institution>
<addr-line><![CDATA[Bogotá ]]></addr-line>
<country>Colombia</country>
</aff>
<aff id="A02">
<institution><![CDATA[,Universidad de Los Andes  ]]></institution>
<addr-line><![CDATA[Bogotá ]]></addr-line>
<country>Colombia</country>
</aff>
<pub-date pub-type="pub">
<day>15</day>
<month>12</month>
<year>2008</year>
</pub-date>
<pub-date pub-type="epub">
<day>15</day>
<month>12</month>
<year>2008</year>
</pub-date>
<volume>42</volume>
<numero>2</numero>
<fpage>183</fpage>
<lpage>207</lpage>
<copyright-statement/>
<copyright-year/>
<self-uri xlink:href="http://www.scielo.org.co/scielo.php?script=sci_arttext&amp;pid=S0034-74262008000200006&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.co/scielo.php?script=sci_abstract&amp;pid=S0034-74262008000200006&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.co/scielo.php?script=sci_pdf&amp;pid=S0034-74262008000200006&amp;lng=en&amp;nrm=iso"></self-uri><abstract abstract-type="short" xml:lang="en"><p><![CDATA[In this paper we compute the square root of the generalized squared total angular momentum operator J for a Dirac particle in the Kerr-Newman metric. The separation constant &lambda; arising from the Chandrasekahr separation ansatz turns out to be the eigenvalue of J. After proving that J is a symmetry operator, we show the completeness of Chandrasekhar ansatz for the Dirac equation in oblate spheroidal coordinates and derive an explicit formula for the time evolution operator e-itH.]]></p></abstract>
<abstract abstract-type="short" xml:lang="es"><p><![CDATA[En este trabajo derivamos la raíz cuadrada del operador generalizado del momento angular para una partícula de Dirac en la métrica de Kerr-Newman. La constante de separación &lambda; introducida por el ansatz de Chandrasekhar resulta ser el valor propio de J. Después de haber mostrado que J es un operador de simetría, probamos la completitud del ansatz de Chandrasekhar para la ecuación de Dirac en coordenadas esferoidales oblongas y derivamos una expresión analítica para el operador de evolución temporal e-itH.]]></p></abstract>
<kwd-group>
<kwd lng="en"><![CDATA[Dirac equation]]></kwd>
<kwd lng="en"><![CDATA[Kerr-Newman metric]]></kwd>
<kwd lng="en"><![CDATA[general relativity]]></kwd>
<kwd lng="es"><![CDATA[Ecuación de Dirac]]></kwd>
<kwd lng="es"><![CDATA[métrica de Kerr-Newman]]></kwd>
<kwd lng="es"><![CDATA[relatividad general]]></kwd>
</kwd-group>
</article-meta>
</front><body><![CDATA[  <font size="2" face="verdana">      <p> <b> <font size="4">     <center> Chandrasekhar ansatz and the generalized total angular momentum operator for the Dirac equation in the Kerr-Newman metric </center> </font> </b> </p>      <p> <b> <font size="3">     <center> El ansatz de Chandrasekhar y el operador generalizado del momento angular para la ecuaci&oacute;n de Dirac en la m&eacute;trica de Kerr-Newman </center> </font> </b> </p>      <p>     <center> DAVIDE BATIC<sup>1</sup>,  HARALD SCHMID<sup>2</sup> </center> </p>      <p> <sup>1</sup>Universidad de Los Andes, Bogot&aacute;, Colombia. Email: <a href="mailto:dbatic@uniandes.edu.co">dbatic@uniandes.edu.co</a>     <br>  <sup>2</sup>Universidad de Los Andes, Bogot&aacute;, Colombia. Email: <a href="mailto:Harald.Schmid@UBH.de">Harald.Schmid@UBH.de</a>     <br> </p>  <hr size="1">      ]]></body>
<body><![CDATA[<p> <b>     <center> Abstract </center> </b> </p>      <p> In this paper we compute the square root of the generalized squared total angular momentum operator <i>J</i> for a Dirac particle in the Kerr-Newman metric. The separation constant <i>&lambda;</i> arising from the Chandrasekahr separation ansatz turns out to be the eigenvalue of <i>J</i>. After proving that <i>J</i> is a symmetry operator, we show the completeness of Chandrasekhar ansatz for the Dirac equation in oblate spheroidal coordinates and derive an explicit formula for the time evolution operator <i>e<sup>-itH</sup></i>. </p>      <p> <b> Key words: </b> Dirac equation, Kerr-Newman metric, general relativity. </p>  <hr size="1">  <i>2000 Mathematics Subject Classification: 83C57, 47B15, 47B25.</i>  <hr size="1">      <p> <b>     <center> Resumen </center> </b> </p>      <p> En este trabajo derivamos la ra&iacute;z cuadrada del operador generalizado del momento angular para una part&iacute;cula de Dirac en la m&eacute;trica de Kerr-Newman. La constante de separaci&oacute;n <i>&lambda;</i> introducida por el ansatz de Chandrasekhar resulta ser el valor propio de <i>J</i>. Despu&eacute;s de haber mostrado que <i>J</i> es un operador de simetr&iacute;a, probamos la completitud del ansatz de Chandrasekhar para la ecuaci&oacute;n de Dirac en coordenadas esferoidales oblongas y derivamos una expresi&oacute;n anal&iacute;tica para el operador de evoluci&oacute;n temporal <i>e<sup>-itH</sup></i>. </p>      <p> <b> Palabras clave: </b> Ecuaci&oacute;n de Dirac, m&eacute;trica de Kerr-Newman, relatividad general. </p>  <hr size="1">      <p> Texto completo disponible en <a href="pdf/rcm/v42n2/v42n2a06.pdf">PDF</a> </p>  <hr size="1">      <p> <b> <font size="3"> References </font> </b> </p>       ]]></body>
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R., <i>Mathematical scattering theory</i>, Vol. 105 of <i>Translations of Mathematical Monographs</i>, American Mathematical Society, Providence, RI, 1992. General theory, Translated from the Russian by J.~R. Schulenberger. &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=000047&pid=S0034-7426200800020000600025&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --><center> <b>(Recibido en marzo de 2008. Aceptado en agosto de 2008)</b> </center> <hr size="1">      <p> Este art&iacute;culo se puede citar en <i>LaTeX</i> utilizando la siguiente referencia bibliogr&aacute;fica de <i>BibTeX</i>: </p> <code><font size="2">@ARTICLE{RCMv42n2a06,    <br>  &nbsp;&nbsp;&nbsp; AUTHOR &nbsp;= {Batic, Davide and Schmid, Harald},    <br>  &nbsp;&nbsp;&nbsp; TITLE &nbsp; = {{Chandrasekhar ansatz and the generalized total angular momentum operator for the Dirac equation in the Kerr-Newman metric}},    <br>  &nbsp;&nbsp;&nbsp; JOURNAL = {Revista Colombiana de Matem&aacute;ticas},    ]]></body>
<body><![CDATA[<br> &nbsp;&nbsp;&nbsp; YEAR &nbsp;&nbsp; = {2008},    <br> &nbsp;&nbsp;&nbsp; volume &nbsp;= {42},    <br> &nbsp;&nbsp;&nbsp; number &nbsp;= {2},    <br> &nbsp;&nbsp;&nbsp; pages &nbsp; = {183-207}    <br> }</font></code>  <hr size="1"> </font>      ]]></body><back>
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