<?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>S0035-001X2012000100013</article-id>
<title-group>
<article-title xml:lang="en"><![CDATA[Hermitian operators and boundary conditions]]></article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Maya-Mendieta]]></surname>
<given-names><![CDATA[M]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Oliveros-Oliveros]]></surname>
<given-names><![CDATA[J]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Teniza-Tetlalmatzi]]></surname>
<given-names><![CDATA[E]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Vargas-Ubera]]></surname>
<given-names><![CDATA[J]]></given-names>
</name>
<xref ref-type="aff" rid="A02"/>
</contrib>
</contrib-group>
<aff id="A01">
<institution><![CDATA[,Benemérita Universidad Autónoma de Puebla Facultad de Ciencias Físico Matemáticas ]]></institution>
<addr-line><![CDATA[ ]]></addr-line>
</aff>
<aff id="A02">
<institution><![CDATA[,Universidad Autónoma de la Ciudad de México Colegio de Ciencia y Tecnología ]]></institution>
<addr-line><![CDATA[ ]]></addr-line>
</aff>
<pub-date pub-type="pub">
<day>00</day>
<month>02</month>
<year>2012</year>
</pub-date>
<pub-date pub-type="epub">
<day>00</day>
<month>02</month>
<year>2012</year>
</pub-date>
<volume>58</volume>
<numero>1</numero>
<fpage>94</fpage>
<lpage>103</lpage>
<copyright-statement/>
<copyright-year/>
<self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_arttext&amp;pid=S0035-001X2012000100013&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_abstract&amp;pid=S0035-001X2012000100013&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_pdf&amp;pid=S0035-001X2012000100013&amp;lng=en&amp;nrm=iso"></self-uri><abstract abstract-type="short" xml:lang="en"><p><![CDATA[The case of the hermeticity of the operators representing the physical observable has received considerable attention in recent years. In this paper we work with a method developed by Morsy and Ata [1] for obtaining Hermitian differential operators independently of the values of the boundary conditions on wave functions. Once obtained these operators, called intrinsically Hermitic operators, we build the Hamiltonian for the harmonic oscillator, hydrogen atom and the potential well of infinite walls. In the first two cases we use the factorization method of ladder operators (also intrinsically Hermitic) and show that results obtained with conventional operators, based on the annulation ofthe wave functions on the boundaries, are preserved. For the infinite well we show that the version of the Hamiltonian intrinsically Hermitic provides a solution to a paradox that appears in a particular wave function.]]></p></abstract>
<abstract abstract-type="short" xml:lang="es"><p><![CDATA[El caso de la hermiticidad de los operadores que representan a los observables ha recibido una atención considerable en los últimos años. En este trabajo tratamos con un método desarrollado por Morsy y Ata [1] para obtener operadores diferenciales hermíticos independientemente de los valores en la frontera que se impongan sobre las funciones de onda. Una vez obtenidos estos operadores, llamados intrínsecamente hermíticos, construimos hamiltonianos para el oscilador armónico, el átomo de hidrógeno y el pozo de potencial de paredes infinitas. En los dos primeros casos utilizamos el método de factorización con operadores de escalera (tambien intrínsecamente hermíticos) y mostramos que se preservan los resultados obtenidos con los operadores convencionales que se basan en la anulación de las funciones de onda en las fronteras. En el caso del pozo infinito mostramos que la version intrínsecamente hermítica del hamiltoniano proporciona una solución a una paradoja que se presenta en una función de onda particular.]]></p></abstract>
<kwd-group>
<kwd lng="en"><![CDATA[Boundary conditions]]></kwd>
<kwd lng="en"><![CDATA[Dirac delta function]]></kwd>
<kwd lng="es"><![CDATA[Condiciones de frontera no nulas]]></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="4">&nbsp;</font></p>     <p align="center"><font face="verdana" size="4"><b>Hermitian operators and boundary conditions</b></font></p>     <p align="center"><font face="verdana" size="2">&nbsp;</font></p>     <p align="center"><font face="verdana" size="2"><b>M. Maya&#150;Mendieta<sup>a</sup>, J. Oliveros&#150;Oliveros<sup>a</sup>, E. Teniza&#150;Tetlalmatzi<sup>a</sup> and J. Vargas&#150;Ubera<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><sup>a</sup> Facultad de Ciencias F&iacute;sico Matem&aacute;ticas, Benem&eacute;rita Universidad Aut&oacute;noma de Puebla. </i></font></p>     <p align="justify"><font face="verdana" size="2"><i><sup>b</sup> Colegio de Ciencia y Tecnolog&iacute;a, Universidad Aut&oacute;noma de la Ciudad de 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">Recibido el 14 de noviembre de 2011.    ]]></body>
<body><![CDATA[<br> Aceptado el 13 de diciembre de 2011.</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">The case of the hermeticity of the operators representing the physical observable has received considerable attention in recent years. In this paper we work with a method developed by Morsy and Ata [1] for obtaining Hermitian differential operators independently of the values of the boundary conditions on wave functions. Once obtained these operators, called intrinsically Hermitic operators, we build the Hamiltonian for the harmonic oscillator, hydrogen atom and the potential well of infinite walls. In the first two cases we use the factorization method of ladder operators (also intrinsically Hermitic) and show that results obtained with conventional operators, based on the annulation ofthe wave functions on the boundaries, are preserved. For the infinite well we show that the version of the Hamiltonian intrinsically Hermitic provides a solution to a paradox that appears in a particular wave function.</font></p>     <p align="justify"><font face="verdana" size="2"><b>Keywords: </b>Boundary conditions; Dirac delta function.</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">El caso de la hermiticidad de los operadores que representan a los observables ha recibido una atenci&oacute;n considerable en los &uacute;ltimos a&ntilde;os. En este trabajo tratamos con un m&eacute;todo desarrollado por Morsy y Ata [1] para obtener operadores diferenciales herm&iacute;ticos independientemente de los valores en la frontera que se impongan sobre las funciones de onda. Una vez obtenidos estos operadores, llamados intr&iacute;nsecamente herm&iacute;ticos, construimos hamiltonianos para el oscilador arm&oacute;nico, el &aacute;tomo de hidr&oacute;geno y el pozo de potencial de paredes infinitas. En los dos primeros casos utilizamos el m&eacute;todo de factorizaci&oacute;n con operadores de escalera (tambien intr&iacute;nsecamente herm&iacute;ticos) y mostramos que se preservan los resultados obtenidos con los operadores convencionales que se basan en la anulaci&oacute;n de las funciones de onda en las fronteras. En el caso del pozo infinito mostramos que la version intr&iacute;nsecamente herm&iacute;tica del hamiltoniano proporciona una soluci&oacute;n a una paradoja que se presenta en una funci&oacute;n de onda particular.</font></p>     <p align="justify"><font face="verdana" size="2"><b>Descriptores: </b>Condiciones de frontera no nulas.</font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     ]]></body>
<body><![CDATA[<p align="justify"><font face="verdana" size="2">PACS: 03.65.&#150;w; 02.30.Hq</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/v58n1/v58n1a13.pdf" target="_blank">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>References</b></font></p>     <!-- ref --><p align="justify"><font face="verdana" size="2">1. M.W. Morsy and M.S. 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