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Phase-space representation for Galilean quantum particles of arbitrary spin

dc.creatorGracia Bondía, José M.
dc.creatorVárilly Boyle, Joseph C.
dc.date.accessioned2022-04-29T15:09:17Z
dc.date.available2022-04-29T15:09:17Z
dc.date.issued1988-09
dc.description.abstractThe phase-space approach to quantization is extended to incorporate spinning particles with Galilean symmetry. The appropriate phase space is the coadjoint orbit R^6 x S^2. From two basic principles, traciality and Galilean covariance, the Weyl symbol calculus is constructed. Then the Galilean-equivariant twisted products of functions on this phase space are identified.es
dc.description.procedenceUCR::Vicerrectoría de Docencia::Ciencias Básicas::Facultad de Ciencias::Escuela de Matemáticaes
dc.identifier.citationhttps://iopscience.iop.org/article/10.1088/0305-4470/21/18/002
dc.identifier.doihttps://doi.org/10.1088/0305-4470/21/18/002
dc.identifier.issn1361-6447
dc.identifier.issn0305-4470
dc.identifier.urihttps://hdl.handle.net/10669/86528
dc.language.isoeng
dc.rightsacceso abierto
dc.sourceJournal of Physics A: Mathematical and General, vol.21(18), pp.L879-L893.es
dc.subjectQuantum mechanics in phase spacees
dc.subjectGalilean symmetryes
dc.subjectFunctionses
dc.titlePhase-space representation for Galilean quantum particles of arbitrary spines
dc.typeartículo originales

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