<?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>S1870-35422015000200007</article-id>
<title-group>
<article-title xml:lang="en"><![CDATA[Symmetry projection, geometry and choice of the basis]]></article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Lemus]]></surname>
<given-names><![CDATA[R.]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Hernández-Castillo]]></surname>
<given-names><![CDATA[A.O.]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
</contrib-group>
<aff id="A01">
<institution><![CDATA[,Universidad Nacional Autónoma de México Instituto de Ciencias Nucleares ]]></institution>
<addr-line><![CDATA[México Distrito Federal]]></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>113</fpage>
<lpage>128</lpage>
<copyright-statement/>
<copyright-year/>
<self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_arttext&amp;pid=S1870-35422015000200007&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_abstract&amp;pid=S1870-35422015000200007&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_pdf&amp;pid=S1870-35422015000200007&amp;lng=en&amp;nrm=iso"></self-uri><abstract abstract-type="short" xml:lang="en"><p><![CDATA[A geometrical point of view of symmetry adapted projection to irreducible subspaces is presented. The projection is applied in two stages. The first step consists in projecting over subspaces spanning irreducible representations (irreps) of the symmetry group, while the second projection is carried out over the irreps of a subgroup defined through a suitable group chain. It is shown that choosing different chains is equivalent to propose alternative bases (passive point of view), while changing the projected function corresponds to the active point of view where the vector to be projected is rotated. Because of the importance of choosing the appropriate basis, an approach based on the concept of invariant operators to obtain the basis for discrete groups is presented. We show that this approach is analogue to the case of continuum groups and it is closely related to the definition of quantum numbers. The importance of these concepts is illustrated through the effect of symmetry breaking. Because of the deep insight into the group theory concepts, we believe the presented viewpoint helps to understand the main ingredients involved in group representation theory using the latest advances in the subject for discrete groups.]]></p></abstract>
<abstract abstract-type="short" xml:lang="es"><p><![CDATA[Se presenta un punto de vista geométrico de la proyección a subespacios que portan representaciones irreducibles. La proyección se lleva a cabo en dos pasos. Primero se efectúa la proyección sobre subespacios que portan representaciones irreducibles del grupo de simetría, para posteriormente efectuar la proyección con respecto a un subgrupo definido a través de una cadena apropiada de subgrupos. Se muestra que la selección de diferentes cadenas es equivalente a proponer bases alternativas (punto de vista pasivo), mientras que el cambio de la función a proyectar equivale al punto de vista activo, donde el vector a proyectar es rotado. Debido a la importancia de seleccionar una base apropiada, se presenta un método de proyección basado en el concepto de operadores invariantes en el caso de grupos discretos. Se muestra que este método es análogo al caso de grupos continuos e íntimamente relacionado con el mismo concepto de número cuántico. La importancia de estos conceptos es ilustrada mediante el concepto de rompimiento de simetría. Creemos que dada la profundidad del marco teórico presentado, este material será de gran ayuda en la comprensión de los conceptos de teoría de representaciones de grupos, en donde se ha incluido la esencia de los últimos métodos de proyección desarrollados para grupos discretos.]]></p></abstract>
<kwd-group>
<kwd lng="en"><![CDATA[Symmetry projection]]></kwd>
<kwd lng="en"><![CDATA[quantum numbers]]></kwd>
<kwd lng="en"><![CDATA[discrete groups]]></kwd>
<kwd lng="en"><![CDATA[eigenfunction approach]]></kwd>
<kwd lng="en"><![CDATA[symmetry breaking]]></kwd>
<kwd lng="es"><![CDATA[Proyección de simetría]]></kwd>
<kwd lng="es"><![CDATA[números cuánticos]]></kwd>
<kwd lng="es"><![CDATA[grupos discretos]]></kwd>
<kwd lng="es"><![CDATA[método de funciones propias]]></kwd>
<kwd lng="es"><![CDATA[rompimiento de simetría]]></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>Symmetry projection, geometry and choice of the basis</b></font></p>  	    <p>&nbsp;</p>  	    <p align="center"><font face="verdana" size="2"><b>R. Lemus and A.O. Hern&aacute;ndez&#45;Castillo</b></font></p>  	    <p>&nbsp;</p>  	    <p align="justify"><font face="verdana" size="2"><i>Instituto de Ciencias Nucleares, Universidad Nacional Aut&oacute;noma de M&eacute;xico, Apartado Postal 70&#45;543, Circuito Exterior, C.U., 04510 M&eacute;xico, D.F., M&eacute;xico.</i></font></p>  	    <p>&nbsp;</p>  	    <p align="justify"><font face="verdana" size="2">Received 04 June 2015;    ]]></body>
<body><![CDATA[<br> 	Accepted 10 August 2015</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">A geometrical point of view of symmetry adapted projection to irreducible subspaces is presented. The projection is applied in two stages. The first step consists in projecting over subspaces spanning irreducible representations (irreps) of the symmetry group, while the second projection is carried out over the irreps of a subgroup defined through a suitable group chain. It is shown that choosing different chains is equivalent to propose alternative bases (passive point of view), while changing the projected function corresponds to the active point of view where the vector to be projected is rotated. Because of the importance of choosing the appropriate basis, an approach based on the concept of invariant operators to obtain the basis for discrete groups is presented. We show that this approach is analogue to the case of continuum groups and it is closely related to the definition of quantum numbers. The importance of these concepts is illustrated through the effect of symmetry breaking. Because of the deep insight into the group theory concepts, we believe the presented viewpoint helps to understand the main ingredients involved in group representation theory using the latest advances in the subject for discrete groups.</font></p>  	    <p align="justify"><font face="verdana" size="2"><b>Keywords:</b> Symmetry projection; quantum numbers; discrete groups; eigenfunction approach; symmetry breaking.</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">Se presenta un punto de vista geom&eacute;trico de la proyecci&oacute;n a subespacios   que portan representaciones irreducibles. La proyecci&oacute;n se lleva a cabo en dos pasos. Primero se efect&uacute;a la proyecci&oacute;n sobre subespacios que portan representaciones irreducibles del grupo de simetr&iacute;a, para posteriormente efectuar la proyecci&oacute;n con respecto a un subgrupo definido a trav&eacute;s de una cadena apropiada de subgrupos. Se muestra que la selecci&oacute;n de diferentes cadenas es equivalente a proponer bases alternativas (punto de vista pasivo), mientras que el cambio de la funci&oacute;n a proyectar equivale al punto de vista activo, donde el vector a proyectar es rotado. Debido a la importancia de seleccionar una base apropiada, se presenta un m&eacute;todo de proyecci&oacute;n basado en el concepto de operadores invariantes en el caso de grupos discretos. Se muestra que este m&eacute;todo es an&aacute;logo al caso de grupos continuos e &iacute;ntimamente relacionado con el mismo concepto de n&uacute;mero cu&aacute;ntico. La importancia de estos conceptos es ilustrada mediante el concepto de rompimiento de simetr&iacute;a. Creemos que dada la profundidad del marco te&oacute;rico presentado, este material ser&aacute; de gran ayuda en la comprensi&oacute;n de los conceptos de teor&iacute;a de representaciones de grupos, en donde se ha incluido la esencia de los &uacute;ltimos m&eacute;todos de proyecci&oacute;n desarrollados para grupos discretos.</font></p>      <p align="justify"><font face="verdana" size="2"><b>Palabras clave:</b> Proyecci&oacute;n de simetr&iacute;a; n&uacute;meros cu&aacute;nticos; grupos discretos; m&eacute;todo de funciones propias; rompimiento de simetr&iacute;a.</font></p>  	    <p>&nbsp;</p>  	    ]]></body>
<body><![CDATA[<p align="justify"><font face="verdana" size="2">PACS: 03.65.Ge; 02.20.&#45;a; 02.20.Bb</font></p>  	    <p>&nbsp;</p>  	    <p align="justify"><font face="verdana" size="2"><a href="/pdf/rmfe/v61n2/v61n2a7.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>Acknowledgments</b></font></p>  	    <p align="justify"><font face="verdana" size="2">This work is partially supported by DGAPA&#45;UNAM under project No. IN109113.</font></p>  	    <p>&nbsp;</p>  	    <p align="justify"><font face="verdana" size="2"><b>References</b></font></p>  	    <!-- ref --><p align="justify"><font face="verdana" size="2">1.&nbsp;F. Albert Cotton, <i>Chemical Applications to Group Theory,</i> John Wiley &amp; Sons, (Inc. New York, 1963).    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8463808&pid=S1870-3542201500020000700001&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></font></p>  	    ]]></body>
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<ref-list>
<ref id="B1">
<label>1</label><nlm-citation citation-type="book">
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<surname><![CDATA[Albert Cotton]]></surname>
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</person-group>
<source><![CDATA[Chemical Applications to Group Theory]]></source>
<year>1963</year>
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<publisher-name><![CDATA[John Wiley & Sons]]></publisher-name>
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