<?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>S0035-001X2015000200009</article-id>
<title-group>
<article-title xml:lang="en"><![CDATA[Transmission and escape in finite superlattices with Gaussian modulation]]></article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Silba-Vélez]]></surname>
<given-names><![CDATA[M. de la Luz]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Pérez-Álvarez]]></surname>
<given-names><![CDATA[R.]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Contreras-Solorio]]></surname>
<given-names><![CDATA[D.A.]]></given-names>
</name>
<xref ref-type="aff" rid="A02"/>
</contrib>
</contrib-group>
<aff id="A01">
<institution><![CDATA[,Universidad Autónoma del Estado de Morelos  ]]></institution>
<addr-line><![CDATA[Cuernavaca Morelos]]></addr-line>
<country>México</country>
</aff>
<aff id="A02">
<institution><![CDATA[,Universidad Autónoma de Zacatecas Unidad Académica de Física ]]></institution>
<addr-line><![CDATA[Zacatecas ]]></addr-line>
<country>México</country>
</aff>
<pub-date pub-type="pub">
<day>00</day>
<month>04</month>
<year>2015</year>
</pub-date>
<pub-date pub-type="epub">
<day>00</day>
<month>04</month>
<year>2015</year>
</pub-date>
<volume>61</volume>
<numero>2</numero>
<fpage>132</fpage>
<lpage>136</lpage>
<copyright-statement/>
<copyright-year/>
<self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_arttext&amp;pid=S0035-001X2015000200009&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_abstract&amp;pid=S0035-001X2015000200009&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_pdf&amp;pid=S0035-001X2015000200009&amp;lng=en&amp;nrm=iso"></self-uri><abstract abstract-type="short" xml:lang="en"><p><![CDATA[We study the transmission and escape energies dependent as a function of the electron energy in superlattices where the barriers height is modulated by a Gaussian function and they are compared with those produced by regular superlattices where all the barriers have the same height. We use for the calculations the effective mass approximation using the transfer matrix formalism. For Gaussian systems with 7 and 9 barriers, the transmission coefficient has passbands with almost perfect transmission. The escape energies E = Er+ i&#915; are situated near these transparency bands but they do not coincide with them and they can be far from the passbands. Er is the electron energy and &#915; describe the width of the states. For these systems the escape states are very wide. In the case of regular systems there are transmission bands which present only resonance peaks with unit value. The escape states are narrow and coincide with these resonances much better than in the case of Gaussian superlattices but the coincidence is not perfect. For 3 barriers where the height of the lateral barriers is reduced gradually, the resonances transform to transparency bands and the width of the escape energies increases. Although there is no coincidence, we associate the increase of width of the escape energies with the formation of transparency bands.]]></p></abstract>
<abstract abstract-type="short" xml:lang="es"><p><![CDATA[Estudiamos la transmisión y energías de escape como función de la energía en superredes donde las alturas de las barreras están moduladas por una función gaussiana y son comparados con los producidos por una superred regular donde todas las alturas de las barreras es la misma. Para los cálculos utilizamos la aproximación de masa efectiva usando el formalismo de matrices de transferencia. Para sistemas gaussianos con 7 y 9 barreras, el coeficiente de transmisión tiene bandas de paso con transmisión casi perfecta. La energías de escape E = Er+ i&#915; están situadas cerca de las bandas de paso. Er es la energía del electrón y &#915; describe el ancho de los estados. Para estos sistemas los estados de escape son amplios. En el caso de los sistemas regulares existen bandas de transmisión que solo presentan picos de resonancia con valor unitario. Los estados de escape son estrechos y coinciden con las resonancias mucho mejor que en el caso de superredes gaussianas pero la coincidencia no es perfecta. Para 3 barreras donde la altura de las barreras laterales se reduce gradualmente, las resonancias se convierten a las bandas de transparencia y la anchura de las energías de escape aumenta. Aunque no hay una coincidencia, asociamos el aumento del ancho de las energías de escape con la formación de bandas de transparencia.]]></p></abstract>
<kwd-group>
<kwd lng="en"><![CDATA[Effective mass]]></kwd>
<kwd lng="en"><![CDATA[transmission]]></kwd>
<kwd lng="en"><![CDATA[escape]]></kwd>
<kwd lng="en"><![CDATA[transfer matrix formalism]]></kwd>
<kwd lng="es"><![CDATA[Masa efectiva]]></kwd>
<kwd lng="es"><![CDATA[transmisión]]></kwd>
<kwd lng="es"><![CDATA[escape]]></kwd>
<kwd lng="es"><![CDATA[formalismo de matrices de transferencia]]></kwd>
</kwd-group>
</article-meta>
</front><body><![CDATA[  	    <p align="justify"><font face="verdana" size="4">Investigaci&oacute;n</font></p>      <p>&nbsp;</p>  	    <p align="center"><font face="verdana" size="4"><b>Transmission and escape in finite superlattices with Gaussian modulation</b></font></p>  	    <p>&nbsp;</p>  	    <p align="center"><font face="verdana" size="2"><b>M. de la Luz Silba&#45;V&eacute;lez<sup>a</sup>, R. P&eacute;rez&#45;&Aacute;lvarez<sup>a</sup>, and D.A. Contreras&#45;Solorio<sup>b</sup></b></font></p>  	    <p>&nbsp;</p>  	    <p align="justify"><font face="verdana" size="2"><i><sup>a</sup> Universidad Aut&oacute;noma del Estado de Morelos, Ave. Universidad 1001, 62209, Cuernavaca, Morelos, M&eacute;xico.</i> e&#45;mail: <a href="mailto:svml@uaem.mx">svml@uaem.mx</a>; <a href="mailto:rpa@uaem.mx">rpa@uaem.mx</a></font>.</p>  	    <p align="justify"><font face="verdana" size="2"><i><sup>b</sup> Unidad Acad&eacute;mica de F&iacute;sica, Universidad Aut&oacute;noma de Zacatecas. Zacatecas, Mexico.</i> e&#45;mail: <a href="mailto:dacs10@yahoo.com.mx">dacs10@yahoo.com.mx</a></font>.</p>  	    <p>&nbsp;</p>  	    ]]></body>
<body><![CDATA[<p align="justify"><font face="verdana" size="2">Received 24 October 2014;    <br> 	accepted 9 February 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">We study the transmission and escape energies dependent as a function of the electron energy in superlattices where the barriers height is modulated by a Gaussian function and they are compared with those produced by regular superlattices where all the barriers have the same height. We use for the calculations the effective mass approximation using the transfer matrix formalism. For Gaussian systems with 7 and 9 barriers, the transmission coefficient has passbands with almost perfect transmission. The escape energies <i>E = E<sub>r</sub></i>+ <i>i&Gamma;</i> are situated near these transparency bands but they do not coincide with them and they can be far from the passbands. <i>E<sub>r</sub></i> is the electron energy and &Gamma; describe the width of the states. For these systems the escape states are very wide. In the case of regular systems there are transmission bands which present only resonance peaks with unit value. The escape states are narrow and coincide with these resonances much better than in the case of Gaussian superlattices but the coincidence is not perfect. For 3 barriers where the height of the lateral barriers is reduced gradually, the resonances transform to transparency bands and the width of the escape energies increases. Although there is no coincidence, we associate the increase of width of the escape energies with the formation of transparency bands.</font></p>      <p align="justify"><font face="verdana" size="2"><b>Keywords:</b> Effective mass; transmission; escape; transfer matrix formalism.</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">Estudiamos la transmisi&oacute;n y energ&iacute;as de escape como funci&oacute;n de la energ&iacute;a en superredes donde las alturas de las barreras est&aacute;n moduladas por una funci&oacute;n gaussiana y son comparados con los producidos por una superred regular donde todas las alturas de las barreras es la misma. Para los c&aacute;lculos utilizamos la aproximaci&oacute;n de masa efectiva usando el formalismo de matrices de transferencia. Para sistemas gaussianos con 7 y 9 barreras, el coeficiente de transmisi&oacute;n tiene bandas de paso con transmisi&oacute;n casi perfecta. La energ&iacute;as de escape <i>E = E<sub>r</sub></i>+ <i>i&Gamma;</i> est&aacute;n situadas cerca de las bandas de paso. <i>E<sub>r</sub></i> es la energ&iacute;a del electr&oacute;n y &Gamma; describe el ancho de los estados. Para estos sistemas los estados de escape son amplios. En el caso de los sistemas regulares existen bandas de transmisi&oacute;n que solo presentan picos de resonancia con valor unitario. Los estados de escape son estrechos y coinciden con las resonancias mucho mejor que en el caso de superredes gaussianas pero la coincidencia no es perfecta. Para 3 barreras donde la altura de las barreras laterales se reduce gradualmente, las resonancias se convierten a las bandas de transparencia y la anchura de las energ&iacute;as de escape aumenta. Aunque no hay una coincidencia, asociamos el aumento del ancho de las energ&iacute;as de escape con la formaci&oacute;n de bandas de transparencia.</font></p>      <p align="justify"><font face="verdana" size="2"><b>Palabras clave:</b> Masa efectiva; transmisi&oacute;n; escape; formalismo de matrices de transferencia.</font></p>  	    ]]></body>
<body><![CDATA[<p>&nbsp;</p>  	    <p align="justify"><font face="verdana" size="2">PACS: 73.21.Cd; 73.40.Gk</font></p>  	    <p>&nbsp;</p>  	    <p align="justify"><font face="verdana" size="2"><a href="/pdf/rmf/v61n2/v61n2a9.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>References</b></font></p>  	    <!-- ref --><p align="justify"><font face="verdana" size="2">1.&nbsp;L. Esaki and R. Tsu, <i>IBM. J. Res. Develop. 14</i> (1970) 61&#45;65.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8402586&pid=S0035-001X201500020000900001&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;I. G&oacute;mez Cuesta, Ph.D. thesis, (Universidad Complutense de Madrid, 2003).    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8402588&pid=S0035-001X201500020000900002&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></font></p>  	    ]]></body>
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