Please use this identifier to cite or link to this item: http://hdl.handle.net/2289/4159
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dc.contributor.authorBhandari, R.-
dc.date.accessioned2011-09-21T11:10:25Z-
dc.date.available2011-09-21T11:10:25Z-
dc.date.issued2011-09-
dc.identifier.citationPhysical Letters A, 2011, Vol.375, p3562en
dc.identifier.issn0375-9601-
dc.identifier.urihttp://hdl.handle.net/2289/4159-
dc.descriptionRestricted Access. An open-access version is available at arXiv.org (one of the alternative locations)en
dc.description.abstractGeneralizing an earlier definition of the noncyclic geometric phase [R. Bhandari, Phys. Lett. A 157 (1991)221], a nonmodular topological phase is defined with reference to a generic time-dependent two-slit interference experiment involving particles with N internal states in which the internal state of both the beams undergoes unitary evolution. A simple proof of the shorter geodesic rule for closure of the open path is presented and several useful new insights into the behavior of the dynamical and geometrical components of the phase shift presented. An effective Hamiltonian interpretation of the observable phase shifts is also presented.en
dc.language.isoenen
dc.publisherElesvier B.V.en
dc.relation.urihttp://arxiv.org/abs/0912.2489en
dc.relation.urihttp://dx.doi.org/10.1016/j.physleta.2011.08.019en
dc.relation.urihttp://adsabs.harvard.edu/abs/2009arXiv0912.2489Ben
dc.rights2011 Elesvier B.V.en
dc.subjectPolarizationen
dc.subjectInterferenceen
dc.subjectGeometric phaseen
dc.subjectTopological Phaseen
dc.subjectBerry's phaseen
dc.titleThe nonmodular topological phase and phase singularitiesen
dc.typeArticleen
Appears in Collections:Research Papers (TP)

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