<?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>S0035-001X2009000100004</article-id>
<title-group>
<article-title xml:lang="en"><![CDATA[Optimization of the diffraction efficiency in non-uniform gratings in sillenite crystals (Bi12SiO20 and Bi12TiO2) considering the variation of fringe period, optical activity and polarization angles in a strong non-linear regime]]></article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname><![CDATA[González]]></surname>
<given-names><![CDATA[G]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Zúñiga]]></surname>
<given-names><![CDATA[A]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Magaña]]></surname>
<given-names><![CDATA[F]]></given-names>
</name>
<xref ref-type="aff" rid="A02"/>
</contrib>
</contrib-group>
<aff id="A01">
<institution><![CDATA[,Instituto Politécnico Nacional Escuela Superior de Física y Matemáticas ]]></institution>
<addr-line><![CDATA[México D.F.]]></addr-line>
<country>México</country>
</aff>
<aff id="A02">
<institution><![CDATA[,Universidad Nacional Autónoma de México Instituto de Física ]]></institution>
<addr-line><![CDATA[México D.F]]></addr-line>
<country>México</country>
</aff>
<pub-date pub-type="pub">
<day>00</day>
<month>02</month>
<year>2009</year>
</pub-date>
<pub-date pub-type="epub">
<day>00</day>
<month>02</month>
<year>2009</year>
</pub-date>
<volume>55</volume>
<numero>1</numero>
<fpage>25</fpage>
<lpage>31</lpage>
<copyright-statement/>
<copyright-year/>
<self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_arttext&amp;pid=S0035-001X2009000100004&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_abstract&amp;pid=S0035-001X2009000100004&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_pdf&amp;pid=S0035-001X2009000100004&amp;lng=en&amp;nrm=iso"></self-uri><abstract abstract-type="short" xml:lang="en"><p><![CDATA[We included the non-uniformity of the grating and of the magnitude and phase of light modulation throughout the sample thickness to optimize the diffraction efficiency. The variation of fringe period, optical activity, birefringence, absorption of light, and polarization angle were considered. We studied strong nonlinear conditions and two crystal orientations one is with the grating vector parallel to the face [001] and the other is with the grating vector perpendicular to the same face. We included applied fields there is a complex relationship among all these parameters, and the prediction of the conditions for the optimum value of the diffraction efficiency is complicated. We report the optimal sample thickness for different situations, considering two wavelengths for reading: green (532 nm) and red (632 nm).]]></p></abstract>
<abstract abstract-type="short" xml:lang="es"><p><![CDATA[Incluimos la no uniformidad de la rejilla y de la magnitud y de la fase de la modulación de la luz a lo largo del espesor de la muestra, para optimizar la eficiencia de difracción, considerando la variación del período de la rejilla, condiciones fuertemente no lineales, actividad óptica, birrefringencia, absorción, ángulo de polarización, campos aplicados y dos orientaciones del cristal: el vector de la rejilla paralelo y perpendicular a la dirección [001]. Existe una relación compleja entre todos estos parámetros y la predicción de las condiciones óptimas para la eficiencia de difracción es complicada. Reportamos el espesor óptimo de la muestra en diferentes circunstancias, utilizando dos diferentes longitudes de onda para la lectura: verde (532 nm) y roja (632 nm).]]></p></abstract>
<kwd-group>
<kwd lng="en"><![CDATA[Photorefractive gratings]]></kwd>
<kwd lng="en"><![CDATA[refractive index]]></kwd>
<kwd lng="en"><![CDATA[beam coupling]]></kwd>
<kwd lng="en"><![CDATA[energy exchange]]></kwd>
<kwd lng="en"><![CDATA[non-linear optics]]></kwd>
<kwd lng="es"><![CDATA[Rejillas fotorrefractivas]]></kwd>
<kwd lng="es"><![CDATA[índice de refracción]]></kwd>
<kwd lng="es"><![CDATA[acoplamiento de haces]]></kwd>
<kwd lng="es"><![CDATA[intercambio de energía]]></kwd>
<kwd lng="es"><![CDATA[óptica no lineal]]></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="2"> &nbsp;</font></p>     <p align="center"><font face="verdana" size="4"><b>Optimization of the diffraction efficiency in non&#150;uniform gratings in sillenite crystals (Bi<sub>12</sub>SiO<sub>20</sub> and Bi<sub>12</sub>TiO<sub>2</sub>) considering the variation of fringe period, optical activity and polarization angles in a strong non&#150;linear regime</b></font></p>     <p align="justify"><font face="verdana" size="2"> &nbsp;</font></p>     <p align="center"><font face="verdana" size="2"><b>G. Gonz&aacute;lez&ordf;, A. Z&uacute;&ntilde;iga&ordf; and F. Maga&ntilde;a<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>&ordf; Escuela Superior de F&iacute;sica y Matem&aacute;ticas, Instituto Polit&eacute;cnico Nacional, M&eacute;xico, </i><i>Edificio 9, Unidad profesional Adolfo L&oacute;pez Mateos, </i><i>M&eacute;xico D.F., 07730, M&eacute;xico.</i></font></p>     <p align="justify"><font face="verdana" size="2"> <i><sup>b</sup> Instituto de F&iacute;sica, Universidad Nacional Aut&oacute;noma de M&eacute;xico, Apartado Postal 20&#150;364, M&eacute;xico D.F 0100, M&eacute;xico, </i>e&#150;mail: <a href="mailto:fernando@fisica.unam.mx">fernando@fisica.unam.mx</a></font></p>     <p align="justify"><font face="verdana" size="2"> &nbsp;</font></p>     <p align="justify"><font face="verdana" size="2"> Recibido el 2 de julio de 2008    ]]></body>
<body><![CDATA[<br>   Aceptado el 27 de enero de 2009</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"> We included the non&#150;uniformity of the grating and of the magnitude and phase of light modulation throughout the sample thickness to optimize the diffraction efficiency. The variation of fringe period, optical activity, birefringence, absorption of light, and polarization angle were considered. We studied strong nonlinear conditions and two crystal orientations one is with the grating vector parallel to the face &#91;001&#93; and the other is with the grating vector perpendicular to the same face. We included applied fields there is a complex relationship among all these parameters, and the prediction of the conditions for the optimum value of the diffraction efficiency is complicated. We report the optimal sample thickness for different situations, considering two wavelengths for reading: green (532 nm) and red (632 nm).</font></p>     <p align="justify"><font face="verdana" size="2"> <b>Keywords: </b>Photorefractive gratings; refractive index; beam coupling; energy exchange; non&#150;linear optics.</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"> Incluimos la no uniformidad de la rejilla y de la magnitud y de la fase de la modulaci&oacute;n de la luz a lo largo del espesor de la muestra, para optimizar la eficiencia de difracci&oacute;n, considerando la variaci&oacute;n del per&iacute;odo de la rejilla, condiciones fuertemente no lineales, actividad &oacute;ptica, birrefringencia, absorci&oacute;n, &aacute;ngulo de polarizaci&oacute;n, campos aplicados y dos orientaciones del cristal: el vector de la rejilla paralelo y perpendicular a la direcci&oacute;n &#91;001&#93;. Existe una relaci&oacute;n compleja entre todos estos par&aacute;metros y la predicci&oacute;n de las condiciones &oacute;ptimas para la eficiencia de difracci&oacute;n es complicada. Reportamos el espesor &oacute;ptimo de la muestra en diferentes circunstancias, utilizando dos diferentes longitudes de onda para la lectura: verde (532 nm) y roja (632 nm).</font></p>     <p align="justify"><font face="verdana" size="2"> <b>Descriptores: </b>Rejillas fotorrefractivas; &iacute;ndice de refracci&oacute;n; acoplamiento de haces; intercambio de energ&iacute;a; &oacute;ptica no lineal.</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: 42.65.&#150;k; 42.70.&#150;a; 42.70.Nq.</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/v55n1/v55n1a4.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>Acknowledgements</b></font></p>     <p align="justify"><font face="verdana" size="2"> We wish to acknowledge partial financial support from Direccion General de Asuntos del Personal Acad&eacute;mico from the Universidad Nacional de M&eacute;xico through grant IN&#150;111807.</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. P. 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