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Quantum interference vs quantum chaos in the nuclear shell model

dc.rights.licensehttp://creativecommons.org/licenses/by/4.0es_MX
dc.creatorAARON GERARDO FERNANDEZ ALARCONes_MX
dc.creatorEDNA MAGDALENA HERNANDEZ GONZALEZes_MX
dc.creatorMATHIEU CHRISTIAN ANNE HAUTEFEUILLEes_MX
dc.creatorEMMANUEL LANDA HERNANDEZes_MX
dc.creatorIRVING OMAR MORALES AGISSes_MX
dc.creatorVICTOR MANUEL VELAZQUEZ AGUILARes_MX
dc.creatorRUBEN YVAN MAARTEN FOSSIONes_MX
dc.creatorCARLOS ERNESTO VARGAS MADRAZOes_MX
dc.creatorALEJANDRO FRANK HOEFLICHes_MX
dc.date2015
dc.date.accessioned2018-12-18T21:34:46Z
dc.date.available2018-12-18T21:34:46Z
dc.identifier.urihttp://repositorio.inger.gob.mx/jspui/handle/20.500.12100/17121
dc.descriptionAbstract: In this paper we study the complexity of the nuclear states in terms of a two body quadupole-quadrupole interaction. Energy distributions and eigenvectors composition exhibit a visible interference pattern which is dependent on the intensity of the interaction. In analogy with optics, the visibility of the interference is related to the purity of the states, therefore, we show that the fluctuations associated with quantum chaos have as their origin the remaining quantum coherence with a visibility magnitude close to 5%.es_MX
dc.descriptionConclusions: In conclusion, we have studied the statistics of energy levels considering the visibility of its distribution as a function of the parameter of quadrupolar interaction. Visibility is an indication of the degree of coherence of nuclear states associated to studied energies. By comparing the visibility to the respective power spectrum, we found a correspondence between the statistics of energy levels and the degree of purity of the nuclear states. The 1/f fluctuations characterizing quantum chaos may be interpreted as a residuum of coherence between nuclear states. The lowest states maintain a high degree of purity, whereas decoherence has almost erased the origin of all intermediate energy states. To define the behavior known as quantum chaos, it is therefore not necessary to manipulate classical or semi-classical images from some dynamic system. Quantum decoherence may be used instead.es_MX
dc.formatAdobe PDFes_MX
dc.languagespaes_MX
dc.publisherIOP Publishinges_MX
dc.relationhttp://iopscience.iop.org/article/10.1088/1742-6596/578/1/012014es_MX
dc.relation.requiresSies_MX
dc.rightsAcceso Abiertoes_MX
dc.sourceJournal of Physics: Conference Series (1742-6588) vol. 578 (2015)es_MX
dc.subjectCIENCIAS FÍSICO MATEMÁTICAS Y CIENCIAS DE LA TIERRAes_MX
dc.subjectFísicaes_MX
dc.subjectFísica teóricaes_MX
dc.subjectTeoría cuántica de camposes_MX
dc.subjectFísica nucleares_MX
dc.subjectTeoría cuánticaes_MX
dc.subjectPhysicses_MX
dc.subjectNuclear physicses_MX
dc.subjectQantum theoryes_MX
dc.titleQuantum interference vs quantum chaos in the nuclear shell modeles_MX
dc.typeArtículoes_MX
dc.audienceResearcherses_MX
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