<?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>S0035-001X2004000600009</article-id>
<title-group>
<article-title xml:lang="en"><![CDATA[Symplectic structures and dynamical symmetry groups]]></article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Torres del Castillo]]></surname>
<given-names><![CDATA[G.F.]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Velázquez Quesada]]></surname>
<given-names><![CDATA[M.P.]]></given-names>
</name>
<xref ref-type="aff" rid="A02"/>
</contrib>
</contrib-group>
<aff id="A01">
<institution><![CDATA[,Universidad Autónoma de Puebla Instituto de Ciencias Departamento de Física Matemática]]></institution>
<addr-line><![CDATA[Puebla ]]></addr-line>
<country>México</country>
</aff>
<aff id="A02">
<institution><![CDATA[,Universidad Autónoma de Puebla Facultad de Ciencias Físico Matemáticas ]]></institution>
<addr-line><![CDATA[Puebla ]]></addr-line>
<country>México</country>
</aff>
<pub-date pub-type="pub">
<day>00</day>
<month>00</month>
<year>2004</year>
</pub-date>
<pub-date pub-type="epub">
<day>00</day>
<month>00</month>
<year>2004</year>
</pub-date>
<volume>50</volume>
<numero>6</numero>
<fpage>608</fpage>
<lpage>613</lpage>
<copyright-statement/>
<copyright-year/>
<self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_arttext&amp;pid=S0035-001X2004000600009&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_abstract&amp;pid=S0035-001X2004000600009&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_pdf&amp;pid=S0035-001X2004000600009&amp;lng=en&amp;nrm=iso"></self-uri><abstract abstract-type="short" xml:lang="en"><p><![CDATA[Apart from the total energy, the two-dimensional isotropic harmonic oscillator possesses three independent constants of motion which, with the standard symplectic structure, generates a dynamical symmetry group isomorphic to SU(2). We show that, by suitably redefining the symplectic structure, any of these three constants of motion can be used as a Hamiltonian, and that the remaining two, together with the total energy, generate a dynamical symmetry group isomorphic to SU(1,1). We also show that the standard energy levels of the quantum two-dimensional isotropic harmonic oscillator and their degeneracies are obtained making use of the appropriate representations of SU(1,1), provided that the canonical commutation relations are modified according to the new symplectic structure. Whereas in classical mechanics the different symplectic structures lead to equivalent formulations of the equations of motion, in quantum mechanics the modifications of the commutation relations should be accompanied by modifications in the interpretation of the formalism in order to obtain results equivalent to those found with the common relations.]]></p></abstract>
<abstract abstract-type="short" xml:lang="es"><p><![CDATA[Aparte de la energía total, el oscilador armónico bidimensional isótropo posee tres constantes de movimiento independientes las cuales, con la estructura simpléctica estándar, generan un grupo de simetría dinámica isomorfo a SU(2). Mostramos que, definiendo adecuadamente la estructura simpléctica, cualquiera de estas tres constantes de movimiento puede ser usada como hamiltoniana y que las dos restantes, junto con la energía total, generan un grupo de simetría dinámica isormorfo a SU(1,1). Mostramos también que los niveles de energía usuales del oscilador armónico bidimensional isótropo cuántico y sus degeneraciones se obtienen haciendo uso de las representaciones apropiadas de SU(1,1), si las relaciones de conmutación canónicas se modifican de acuerdo con la nueva estructura simpléctica. Mientras que en la mecánica clásica las diferentes estructuras simplécticas llevan a formulaciones equivalentes de las ecuaciones de movimiento, en la mecánica cuántica, la modificación de las relaciones de conmutación debe estar acompañada de modificaciones en la interpretación del formalismo para obtener resultados equivalentes a los que se hallan con las relaciones usuales.]]></p></abstract>
<kwd-group>
<kwd lng="en"><![CDATA[Dynamical symmetry groups]]></kwd>
<kwd lng="en"><![CDATA[symplectic structures]]></kwd>
<kwd lng="en"><![CDATA[quantization]]></kwd>
<kwd lng="es"><![CDATA[Grupos de simetría dinámica]]></kwd>
<kwd lng="es"><![CDATA[estructuras simplécticas]]></kwd>
<kwd lng="es"><![CDATA[cuantización]]></kwd>
</kwd-group>
</article-meta>
</front><body><![CDATA[  	    <p align="justify"><font face="verdana" size="4">Investigaci&oacute;n</font></p>      <p align="justify">&nbsp;</p>     <p align="center"><font face="verdana" size="4"><b>Symplectic structures and dynamical symmetry groups</b></font></p>      <p align="center">&nbsp;</p>     <p align="center"><font face="verdana" size="2"><b>G.F. Torres del Castillo<sup>a</sup> and M.P. Vel&aacute;zquez Quesada<sup>b</sup></b></font></p>     <p align="center">&nbsp;</p>      <p align="justify"><font face="verdana" size="2"><i><sup>a</sup> Departamento de F&iacute;sica Matem&aacute;tica, Instituto de Ciencias, Universidad Aut&oacute;noma de Puebla, 72570 Puebla, Pue., M&eacute;xico</i></font>.</p>     <p align="justify"><font face="verdana" size="2"><i> <sup>b</sup> Facultad de Ciencias F&iacute;sico Matem&aacute;ticas, Universidad Aut&oacute;noma de Puebla, Apartado postal 1152, 72001 Puebla, Pue., M&eacute;xico</i></font>.</p>     <p align="justify">&nbsp;</p>     ]]></body>
<body><![CDATA[<p align="justify"><font face="verdana" size="2">Recibido el 29 de enero de 2004.    <br> Aceptado el de de 2004</font></p>     <p align="justify">&nbsp;</p>     <p align="justify"><font face="verdana" size="2"><b>Abstract</b></font></p>     <p align="justify"><font face="verdana" size="2">Apart from the total energy, the two&#45;dimensional isotropic harmonic oscillator possesses three independent constants of motion which, with the standard symplectic structure, generates a dynamical symmetry group isomorphic to SU(2). We show that, by suitably redefining the symplectic structure, any of these three constants of motion can be used as a Hamiltonian, and that the remaining two, together with the total energy, generate a dynamical symmetry group isomorphic to SU(1,1). We also show that the standard energy levels of the quantum two&#45;dimensional isotropic harmonic oscillator and their degeneracies are obtained making use of the appropriate representations of SU(1,1), provided that the canonical commutation relations are modified according to the new symplectic structure. Whereas in classical mechanics the different symplectic structures lead to equivalent formulations of the equations of motion, in quantum mechanics the modifications of the commutation relations should be accompanied by modifications in the interpretation of the formalism in order to obtain results equivalent to those found with the common relations.</font></p>  	    <p align="justify"><font face="verdana" size="2"><b>Keywords:</b> Dynamical symmetry groups; symplectic structures; quantization.</font></p>  	    <p align="justify">&nbsp;</p> 	    <p align="justify"><font face="verdana" size="2"><b>Resumen</b></font></p>     <p align="justify"><font face="verdana" size="2">Aparte de la energ&iacute;a total, el oscilador arm&oacute;nico bidimensional is&oacute;tropo posee tres constantes de movimiento independientes las cuales, con la estructura simpl&eacute;ctica est&aacute;ndar, generan un grupo de simetr&iacute;a din&aacute;mica isomorfo a SU(2). Mostramos que, definiendo adecuadamente la estructura simpl&eacute;ctica, cualquiera de estas tres constantes de movimiento puede ser usada como hamiltoniana y que las dos restantes, junto con la energ&iacute;a total, generan un grupo de simetr&iacute;a din&aacute;mica isormorfo a SU(1,1). Mostramos tambi&eacute;n que los niveles de energ&iacute;a usuales del oscilador arm&oacute;nico bidimensional is&oacute;tropo cu&aacute;ntico y sus degeneraciones se obtienen haciendo uso de las representaciones apropiadas de SU(1,1), si las relaciones de conmutaci&oacute;n can&oacute;nicas se modifican de acuerdo con la nueva estructura simpl&eacute;ctica. Mientras que en la mec&aacute;nica cl&aacute;sica las diferentes estructuras simpl&eacute;cticas llevan a formulaciones equivalentes de las ecuaciones de movimiento, en la mec&aacute;nica cu&aacute;ntica, la modificaci&oacute;n de las relaciones de conmutaci&oacute;n debe estar acompa&#241;ada de modificaciones en la interpretaci&oacute;n del formalismo para obtener resultados equivalentes a los que se hallan con las relaciones usuales.</font></p>      <p align="justify"><font face="verdana" size="2"><b>Descriptores:</b> Grupos de simetr&iacute;a din&aacute;mica; estructuras simpl&eacute;cticas; cuantizaci&oacute;n.</font></p>     ]]></body>
<body><![CDATA[<p align="justify">&nbsp;</p>      <p align="justify"><font face="verdana" size="2">PACS: 45.20.Jj; 03.65.Fd</font></p>     <p align="justify">&nbsp;</p>     <p align="justify"><font face="verdana" size="2"><a href="/pdf/rmf/v50n6/v50n6a9.pdf" target="_blank">DESCARGAR ART&Iacute;CULO EN FORMATO PDF</a></font></p>  	    <p align="justify">&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;G.F. Torres del Castillo and G. Mendoza Torres, <i>Rev. Mex. Fis.</i> <b>49</b> (2003) 445.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8306811&pid=S0035-001X200400060000900001&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;M. Montesinos, <i>Phys. Rev. A</i> <b>68</b> (2003) 014101.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8306813&pid=S0035-001X200400060000900002&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></font></p>  	    ]]></body>
<body><![CDATA[<!-- ref --><p align="justify"><font face="verdana" size="2">3.&nbsp;H.V. McIntosh, <i>Am. J. Phys.</i> <b>27</b> (1959) 620.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8306815&pid=S0035-001X200400060000900003&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">4.&nbsp;H. Goldstein, <i>Classical Mechanics,</i> 2nd ed., (Addison&#45;Wesley, Reading, Mass., 1980).    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8306817&pid=S0035-001X200400060000900004&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">5.&nbsp;G.F. Torres del Castillo and J.L. Calvario Ac&oacute;cal, <i>Rev. Mex. F&iacute;s.</i> <b>43</b> (1997) 649.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8306819&pid=S0035-001X200400060000900005&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">6.&nbsp;G.F. Torres del Castillo, <i>3&#45;D Spinors, Spin&#45;Weighted Functions and their Applications,</i> (Birkh&auml;user, Boston, 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=8306821&pid=S0035-001X200400060000900006&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">7.&nbsp;L.I. Schiff, <i>Quantum Mechanics,</i> 3rd ed., (McGraw&#45;Hill, New York, 1968), Chap. 7.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8306823&pid=S0035-001X200400060000900007&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></font></p>  	    ]]></body>
<body><![CDATA[<!-- ref --><p align="justify"><font face="verdana" size="2">8.&nbsp;O.L. de Lange and R.E. Raab, <i>Operator Methods in Quantum Mechanics,</i> (Oxford University Press, Oxford, 1991).    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8306825&pid=S0035-001X200400060000900008&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">9. G.F. Torres del Castillo, "The Lagrangians of a one&#45;dimensional mechanical system", <i>Rev. Mex. F&iacute;s.</i> <b>50</b> (2004)</font><font face="verdana" size="2"> 379.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8306827&pid=S0035-001X200400060000900009&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">10.&nbsp;M. Moshinsky and Yu.F. Smirnov, <i>The Harmonic Oscillator in Modern Physics,</i> Contemporary Concepts in Physics Series, Vol. 9, (Harwood, Amsterdam, 1996), Chap. VII.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8306829&pid=S0035-001X200400060000900010&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">11.&nbsp;G.F. Torres del Castillo, <i>Rev. Mex. Fis.</i> <b>40</b> (1994) 195.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8306831&pid=S0035-001X200400060000900011&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">12.&nbsp;B.G. Adams, J. Cizek and J. Paldus, in <i>Advances in Quantum Chemistry,</i> Vol. 19, Per&#45;Olov L&ouml;wdin, ed., (Academic Press, New York, 1987), reprinted in <i>Dynamical Groups and Spectrum Generating Algebras,</i> Vol. 1, (World Scientific, Singapore,</font> <font face="verdana" size="2">1988).    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8306833&pid=S0035-001X200400060000900012&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></font></p>     ]]></body>
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