<?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>1870-3542</journal-id>
<journal-title><![CDATA[Revista mexicana de física E]]></journal-title>
<abbrev-journal-title><![CDATA[Rev. mex. fís. E]]></abbrev-journal-title>
<issn>1870-3542</issn>
<publisher>
<publisher-name><![CDATA[Sociedad Mexicana de Física]]></publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id>S1870-35422015000200006</article-id>
<title-group>
<article-title xml:lang="es"><![CDATA[Espinores de Weyl y el formalismo de helicidad]]></article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Díaz Cruz]]></surname>
<given-names><![CDATA[J.L.]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Larios]]></surname>
<given-names><![CDATA[B.]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Meza Aldama]]></surname>
<given-names><![CDATA[O.]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Reyes Pérez]]></surname>
<given-names><![CDATA[J.]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
</contrib-group>
<aff id="A01">
<institution><![CDATA[,Benemérita Universidad Autónoma de Puebla Facultad de Ciencias Físico-Matemáticas ]]></institution>
<addr-line><![CDATA[Puebla ]]></addr-line>
<country>México</country>
</aff>
<pub-date pub-type="pub">
<day>00</day>
<month>12</month>
<year>2015</year>
</pub-date>
<pub-date pub-type="epub">
<day>00</day>
<month>12</month>
<year>2015</year>
</pub-date>
<volume>61</volume>
<numero>2</numero>
<fpage>104</fpage>
<lpage>112</lpage>
<copyright-statement/>
<copyright-year/>
<self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_arttext&amp;pid=S1870-35422015000200006&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_abstract&amp;pid=S1870-35422015000200006&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_pdf&amp;pid=S1870-35422015000200006&amp;lng=en&amp;nrm=iso"></self-uri><abstract abstract-type="short" xml:lang="es"><p><![CDATA[En este trabajo revisamos la formulación original de la ecuación relativista para partículas con espín (1/2). Tradicionalmente ("a la Dirac"), se propone que la "raíz cuadrada" de la ecuación de Klein Gordon (K-G) involucra un espinor (de Dirac) de 4 componentes y en el límite no relativista se puede escribir como 2 ecuaciones para dos espinores de 2 componentes. Por otra parte, existe el formalismo de Weyl, en el cual de entrada se trabaja con espinores de Weyl de 2 componentes, los cuales son los objetos fundamentales en el formalismo de helicidad. En este trabajo rederivamos las ecuaciones de Weyl directamente, partiendo de la ecuación de K-G, asimismo se introduce la interacción electromagnética con los espinores de Weyl. Como un ejemplo de aplicación de dicho formalismo, se calcula la dispersión de Compton usando los métodos de helicidad.]]></p></abstract>
<abstract abstract-type="short" xml:lang="en"><p><![CDATA[In this work we give a review of the original formulation of the relativistic wave equation for particles with spin one-half. Traditionally (Ã la Dirac), it's proposed that the "square root" of the Klein-Gordon (K-G) equation involves a 4 component (Dirac) spinor and in the non-relativistic limit it can be written as 2 equations for two 2 component spinors. On the other hand, there exists Weyl's formalism, in which one works from the beginning with 2 component Weyl spinors, which are the fundamental objects of the helicity formalism. In this work we rederive Weyl's equations directly, starting from K-G equation We also introduce the electromagnetic interaction with the Weyl spinors. As an example of the use of that formalism, we calculate Compton scattering using the helicity methods.]]></p></abstract>
<kwd-group>
<kwd lng="es"><![CDATA[Espinores de Weyl]]></kwd>
<kwd lng="es"><![CDATA[formalismo de helicidad]]></kwd>
<kwd lng="es"><![CDATA[dispersión de Compton]]></kwd>
<kwd lng="en"><![CDATA[Weyl spinors]]></kwd>
<kwd lng="en"><![CDATA[helicity formalism]]></kwd>
<kwd lng="en"><![CDATA[Compton scattering]]></kwd>
</kwd-group>
</article-meta>
</front><body><![CDATA[  	    <p align="justify"><font face="verdana" size="4">Educaci&oacute;n</font></p>  	    <p>&nbsp;</p>  	    <p align="center"><font face="verdana" size="4"><b>Espinores de Weyl y el formalismo de helicidad</b></font></p>  	    <p>&nbsp;</p>  	    <p align="center"><font face="verdana" size="2"><b>J.L. D&iacute;az Cruz, B. Larios, O. Meza Aldama y J. Reyes P&eacute;rez</b></font></p>  	    <p>&nbsp;</p>  	    <p align="justify"><font face="verdana" size="2"><i>Facultad de Ciencias F&iacute;sico&#45;Matem&aacute;ticas, Benem&eacute;rita Universidad Aut&oacute;noma de Puebla, Av. San Claudio y 18 Sur, C. U. 72570 Puebla, M&eacute;xico.</i></font></p>  	    <p>&nbsp;</p>  	    <p align="justify"><font face="verdana" size="2">Received 27 March 2015;    ]]></body>
<body><![CDATA[<br> 	Accepted 28 July 2015</font></p>  	    <p>&nbsp;</p>  	    <p align="justify"><font face="verdana" size="2"><b>Resumen</b></font></p>  	    <p align="justify"><font face="verdana" size="2">En este trabajo revisamos la formulaci&oacute;n original de la ecuaci&oacute;n relativista para part&iacute;culas con esp&iacute;n (1/2). Tradicionalmente ("a la Dirac"), se propone que la "ra&iacute;z cuadrada" de la ecuaci&oacute;n de Klein Gordon (K&#45;G) involucra un espinor (de Dirac) de 4 componentes y en el l&iacute;mite no relativista se puede escribir como 2 ecuaciones para dos espinores de 2 componentes. Por otra parte, existe el formalismo de Weyl, en el cual de entrada se trabaja con espinores de Weyl de 2 componentes, los cuales son los objetos fundamentales en el formalismo de helicidad. En este trabajo rederivamos las ecuaciones de Weyl directamente, partiendo de la ecuaci&oacute;n de K&#45;G, asimismo se introduce la interacci&oacute;n electromagn&eacute;tica con los espinores de Weyl. Como un ejemplo de aplicaci&oacute;n de dicho formalismo, se calcula la dispersi&oacute;n de Compton usando los m&eacute;todos de helicidad.</font></p>  	    <p align="justify"><font face="verdana" size="2"><b>Descriptores:</b> Espinores de Weyl; formalismo de helicidad; dispersi&oacute;n de Compton.</font></p>  	    <p>&nbsp;</p>  	    <p align="justify"><font face="verdana" size="2"><b>Abstract</b></font></p>  	    <p align="justify"><font face="verdana" size="2">In this work we give a review of the original formulation of the relativistic wave equation for particles with spin one&#45;half. Traditionally (<i>&#195; la Dirac),</i> it's proposed that the "square root" of the Klein&#45;Gordon (K&#45;G) equation involves a 4 component (Dirac) spinor and in the non&#45;relativistic limit it can be written as 2 equations for two 2 component spinors. On the other hand, there exists Weyl's formalism, in which one works from the beginning with 2 component Weyl spinors, which are the fundamental objects of the helicity formalism. In this work we rederive Weyl's equations directly, starting from K&#45;G equation We also introduce the electromagnetic interaction with the Weyl spinors. As an example of the use of that formalism, we calculate Compton scattering using the helicity methods.</font></p>  	    <p align="justify"><font face="verdana" size="2"><b>Keywords:</b> Weyl spinors; helicity formalism; Compton scattering.</font></p>  	    <p>&nbsp;</p>  	    ]]></body>
<body><![CDATA[<p align="justify"><font face="verdana" size="2">PACS: 03.65.Pm; 11.80.Cr</font></p>  	    <p>&nbsp;</p>  	    <p align="justify"><font face="verdana" size="2"><a href="/pdf/rmfe/v61n2/v61n2a6.pdf" target="_blank">DESCARGAR ART&Iacute;CULO EN FORMATO PDF</a></font></p>     <p>&nbsp;</p>  	    <p align="justify"><font face="verdana" size="2"><b>Referencias</b></font></p>  	    <!-- ref --><p align="justify"><font face="verdana" size="2">1.&nbsp;T. D. Lee y C. N. Yang, <i>Phys. Rev.</i> <b>104</b> (1956) 254.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8463726&pid=S1870-3542201500020000600001&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></font></p>     <!-- ref --><p align="justify"><font face="verdana" size="2">2.&nbsp;T. D. Lee y C. N. Yang, <i>Phys. 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