<?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>S0035-001X2006001000007</article-id>
<title-group>
<article-title xml:lang="en"><![CDATA[DWBA-calculations of elastic scattering, fusion and breakup cross sections for reactions involving weakly bound stable projectiles around the barrier energy]]></article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Gómez Camacho]]></surname>
<given-names><![CDATA[A.]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Aguilera]]></surname>
<given-names><![CDATA[E.F.]]></given-names>
</name>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Quiroz]]></surname>
<given-names><![CDATA[E.M.]]></given-names>
</name>
</contrib>
</contrib-group>
<aff id="A01">
<institution><![CDATA[,Instituto Nacional de Investigaciones Nucleares Departamento del Acelerador ]]></institution>
<addr-line><![CDATA[México D.F.]]></addr-line>
</aff>
<pub-date pub-type="pub">
<day>00</day>
<month>11</month>
<year>2006</year>
</pub-date>
<pub-date pub-type="epub">
<day>00</day>
<month>11</month>
<year>2006</year>
</pub-date>
<volume>52</volume>
<fpage>30</fpage>
<lpage>37</lpage>
<copyright-statement/>
<copyright-year/>
<self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_arttext&amp;pid=S0035-001X2006001000007&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_abstract&amp;pid=S0035-001X2006001000007&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_pdf&amp;pid=S0035-001X2006001000007&amp;lng=en&amp;nrm=iso"></self-uri><abstract abstract-type="short" xml:lang="en"><p><![CDATA[A simultaneous Distorted Wave Born Approximation calculation of elastic scattering, fusion and breakup cross sections for energies above and below the Coulomb barrier energy is presented for reactions involving weakly bound projectiles on heavy targets. In the approach, a Woods-Saxon optical potential U is used where its imaginary part W is split into a volume part W F which is only responsible for fusion absorption and a surface part Wdr which accounts for direct reactions. The fusion and direct reaction cross sections are calculated in terms of W F and W DR respectively. The optical potential parameters are determined from a simultaneous <img border=0 src="../../../../../img/revistas/rmf/v52s4/a7s1.jpg">-analysis of recent experimental data of elastic scattering and fusion cross sections. From this, energy dependent forms for W F (E) and W DR (E) can be determined and by the dispersion relation the corresponding real polarization potentials V F (E) and V DR (E) are also found. The appearance or absence of the threshold anomaly can therefore be extracted from these energy dependent forms. By turning on and off the potentials responsible for breakup reactions (V DR and W DR) the effect of breakup on fusion can be studied. So, regions of suppresion and of enhancement around the barrier energy can be determined for the nuclear systems under study.]]></p></abstract>
<abstract abstract-type="short" xml:lang="es"><p><![CDATA[Dentro de la aproximación de ondas distorsionadas de Born, se hace un estudio simultáneo de reacciones de dispersión elástica, fusión y de rompimiento del projectil conocido como breakup para reacciones nucleares que involucran projectiles debilmente ligados con blancos pesados. Se utilizan potenciales de Woods-Saxon U en los que la parte imaginaria W que es responsable de todos los procesos de absorción es dividida en dos partes, una W F responsable solo de los procesos de fusión y otra W DR de los demás procesos, es decir de las reacciones directas. Los parámetros de tales potenciales serán determinados através de un ajuste simultáneo de los datos experimentales de fusión y de dispersion elástica. Se formulan entonces formas dependientes de la energía para W F y W DR através de las cuales de pueden determinar las partes reales de los potenciales de polarización V F y V DR usando la relación de dispersión. Del comportamiento con la energía de estas cuatro formas puede entonces determinarse la presencia o ausencia de la anomalía de umbral para el potencial de fusión y de reacciones directas respectivamente y en consecuencia del potencial total de absorción W. Finalmente considerando o anulando los potenciales V DR y W DR se realiza un estudio de la influencia que el proceso de rompimiento del projectil (breakup) tiene sobre el de fusión.]]></p></abstract>
<kwd-group>
<kwd lng="en"><![CDATA[Nuclear reactions]]></kwd>
<kwd lng="en"><![CDATA[exotic nuclei]]></kwd>
<kwd lng="en"><![CDATA[threshold anomaly]]></kwd>
<kwd lng="es"><![CDATA[Reacciones nucleares]]></kwd>
<kwd lng="es"><![CDATA[núcleos exóticos]]></kwd>
<kwd lng="es"><![CDATA[anomalía de umbral]]></kwd>
</kwd-group>
</article-meta>
</front><body><![CDATA[ <p align="center"><font face="verdana" size="4"><b>DWBA&#150;calculations of elastic scattering, fusion and breakup cross sections for reactions involving weakly bound stable projectiles around the barrier energy</b></font></p>     <p align="center"><font face="verdana" size="2">&nbsp;</font></p>     <p align="center"><font face="verdana" size="2"><b>A. G&oacute;mez Camacho, E.F. Aguilera, and E.M. Quiroz</b></font></p>     <p align="center"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2"><i>Departamento del Acelerador, Instituto Nacional de Investigaciones Nucleares, Apartado Postal 18&#150;1027, 11801, M&eacute;xico, D.F. e&#150;mail: <a href="mailto:agc@nuclear.inin.mx" target="_blank">agc@nuclear.inin.mx</a></i></font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2">Recibido el 13 de febrero de 2006    <br>   Aceptado el 8 de agosto de 2006</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>     ]]></body>
<body><![CDATA[<p align="justify"><font face="verdana" size="2">A simultaneous Distorted Wave Born Approximation calculation of elastic scattering, fusion and breakup cross sections for energies above and below the Coulomb barrier energy is presented for reactions involving weakly bound projectiles on heavy targets. In the approach, a Woods&#150;Saxon optical potential <i>U </i>is used where its imaginary part <i>W </i>is split into a volume part <i>W<sub>F </sub></i>which is only responsible for fusion absorption and a surface part <i>Wdr </i>which accounts for direct reactions. The fusion and direct reaction cross sections are calculated in terms of <i>W<i><sub>F</sub></i></i> and <i>W<sub>DR </sub></i>respectively. The optical potential parameters are determined from a simultaneous <img src="/img/revistas/rmf/v52s4/a7s1.jpg">&#150;analysis of recent experimental data of elastic scattering and fusion cross sections. From this, energy dependent forms for <i>W<i><sub>F</sub></i> (E) </i>and <i>W<i><sub>DR </sub></i>(E) </i>can be determined and by the dispersion relation the corresponding real polarization potentials <i>V<i><sub>F</sub></i> (E) </i>and <i>V<i><sub>DR</sub></i> (E) </i>are also found. The appearance or absence of the threshold anomaly can therefore be extracted from these energy dependent forms. By turning on and off the potentials responsible for breakup reactions <i>(V<i><sub>DR</sub></i></i> and <i>W<i><sub>DR</sub></i>) </i>the effect of breakup on fusion can be studied. So, regions of suppresion and of enhancement around the barrier energy can be determined for the nuclear systems under study.</font></p>     <p align="justify"><font face="verdana" size="2"><b>Keywords: </b>Nuclear reactions; exotic nuclei; threshold anomaly.</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">Dentro de la aproximaci&oacute;n de ondas distorsionadas de Born, se hace un estudio simult&aacute;neo de reacciones de dispersi&oacute;n el&aacute;stica, fusi&oacute;n y de rompimiento del projectil conocido como breakup para reacciones nucleares que involucran projectiles debilmente ligados con blancos pesados. Se utilizan potenciales de Woods&#150;Saxon <i>U </i>en los que la parte imaginaria <i>W </i>que es responsable de todos los procesos de absorci&oacute;n es dividida en dos partes, una <i>W<sub>F</sub></i><i> </i>responsable solo de los procesos de fusi&oacute;n y otra <i>W<i><sub>DR</sub></i></i> de los dem&aacute;s procesos, es decir de las reacciones directas. Los par&aacute;metros de tales potenciales ser&aacute;n determinados atrav&eacute;s de un ajuste simult&aacute;neo de los datos experimentales de fusi&oacute;n y de dispersion el&aacute;stica. Se formulan entonces formas dependientes de la energ&iacute;a para <i>W<i><sub>F</sub></i></i> y <i>W<i><sub>DR</sub></i></i> atrav&eacute;s de las cuales de pueden determinar las partes reales de los potenciales de polarizaci&oacute;n <i>V<i><sub>F</sub></i> y V<i><sub>DR</sub></i></i> usando la relaci&oacute;n de dispersi&oacute;n. Del comportamiento con la energ&iacute;a de estas cuatro formas puede entonces determinarse la presencia o ausencia de la anomal&iacute;a de umbral para el potencial de fusi&oacute;n y de reacciones directas respectivamente y en consecuencia del potencial total de absorci&oacute;n <i>W. </i>Finalmente considerando o anulando los potenciales <i>V<i><sub>DR</sub></i></i> y <i>W<i><sub>DR</sub></i></i> se realiza un estudio de la influencia que el proceso de rompimiento del projectil (breakup) tiene sobre el de fusi&oacute;n.</font></p>     <p align="justify"><font face="verdana" size="2"><b>Descriptores: </b>Reacciones nucleares; n&uacute;cleos ex&oacute;ticos; anomal&iacute;a de umbral.</font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2">PACS: 24.10.&#150;i; 25.70.Jj; 23.23.+x; 56.65.Dy</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/v52s4/v52s4a7.pdf">DESCARGAR ART&Iacute;CULO EN FORMATO PDF</a></font></p>     ]]></body>
<body><![CDATA[<p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2"><b>Acknowledgments</b></font></p>     <p align="justify"><font face="verdana" size="2">This work has been supported in part by CONACYT under project 44251.</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.G. Hansen <i>et al., Annu. Rev: Nucl. Part. Sci. </i><b>45 </b>(1995) 591.</font>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8330490&pid=S0035-001X200600100000700001&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --><!-- ref --><p align="justify"><font face="verdana" size="2">2. J.J. Kolata <i>et al., Phys. 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