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dc.contributor.authorDe Lima, Emanuel F.-
dc.contributor.authorRamos, Tárcius N.-
dc.contributor.authorDe Carvalho, R. Egydio-
dc.date.accessioned2014-05-27T11:27:33Z-
dc.date.accessioned2016-10-25T18:41:46Z-
dc.date.available2014-05-27T11:27:33Z-
dc.date.available2016-10-25T18:41:46Z-
dc.date.issued2013-01-03-
dc.identifierhttp://dx.doi.org/10.1103/PhysRevE.87.014901-
dc.identifier.citationPhysical Review E - Statistical, Nonlinear, and Soft Matter Physics, v. 87, n. 1, 2013.-
dc.identifier.issn1539-3755-
dc.identifier.issn1550-2376-
dc.identifier.urihttp://hdl.handle.net/11449/74344-
dc.identifier.urihttp://acervodigital.unesp.br/handle/11449/74344-
dc.description.abstractThe dissociation dynamics of heteronuclear diatomic molecules induced by infrared laser pulses is investigated within the framework of the classical driven Morse oscillator. The interaction between the molecule and the laser field described in the dipole formulation is given by the product of a time-dependent external field with a position-dependent permanent dipole function. The effects of changing the spatial range of the dipole function in the classical dissociation dynamics of large ensembles of trajectories are studied. Numerical calculations have been performed for distinct amplitudes and carrier frequencies of the external pulses and also for ensembles with different initial energies. It is found that there exist a set of values of the dipole range for which the dissociation probability can be completely suppressed. The dependence of the dissociation on the dipole range is explained through the examination of the Fourier series coefficients of the dipole function in the angle variable of the free system. In particular, the suppression of dissociation corresponds to dipole ranges for which the Fourier coefficients associated with nonlinear resonances are null and the chaotic region in the phase space is reduced to thin layers. In this context, it is shown that the suppression of dissociation of heteronuclear molecules for certain frequencies of the external field is a consequence of the finite range of the corresponding permanent dipole. © 2013 American Physical Society.en
dc.language.isoeng-
dc.sourceScopus-
dc.subjectAngle variables-
dc.subjectCarrier frequency-
dc.subjectChaotic regions-
dc.subjectClassical dynamics-
dc.subjectDissociation dynamics-
dc.subjectDissociation probability-
dc.subjectExternal fields-
dc.subjectFourier coefficients-
dc.subjectHeteronuclear diatomic molecule-
dc.subjectHeteronuclear molecules-
dc.subjectInitial energy-
dc.subjectLaser fields-
dc.subjectMolecular dissociation-
dc.subjectMorse oscillator-
dc.subjectNonlinear resonance-
dc.subjectNumerical calculation-
dc.subjectPermanent dipoles-
dc.subjectPhase spaces-
dc.subjectThin layers-
dc.subjectTime-dependent-
dc.subjectDynamics-
dc.subjectFourier analysis-
dc.subjectMolecules-
dc.subjectPhase space methods-
dc.subjectDissociation-
dc.titleRole of the range of the dipole function in the classical dynamics of molecular dissociationen
dc.typeoutro-
dc.contributor.institutionUniversidade Estadual Paulista (UNESP)-
dc.description.affiliationInstituto de Geociências e Ciências Exatas UNESP-Univ Estadual Paulista, Rio Claro, São-Paulo 13506-900-
dc.description.affiliationUnespInstituto de Geociências e Ciências Exatas UNESP-Univ Estadual Paulista, Rio Claro, São-Paulo 13506-900-
dc.identifier.doi10.1103/PhysRevE.87.014901-
dc.identifier.wosWOS:000314102900026-
dc.rights.accessRightsAcesso restrito-
dc.identifier.file2-s2.0-84872326396.pdf-
dc.relation.ispartofPhysical Review E: Statistical, Nonlinear, and Soft Matter Physics-
dc.identifier.scopus2-s2.0-84872326396-
Appears in Collections:Artigos, TCCs, Teses e Dissertações da Unesp

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