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dc.contributor.authorLeón, Juan-
dc.date.accessioned2014-09-29T10:37:26Z-
dc.date.available2014-09-29T10:37:26Z-
dc.date.issued1997-
dc.identifierdoi: 10.1088/0305-4470/30/13/027-
dc.identifierissn: 0305-4470-
dc.identifier.citationJournal of Physics A: Mathematical and General 30: 4791 (1997)-
dc.identifier.urihttp://hdl.handle.net/10261/102626-
dc.description.abstractAbstract. A suitable operator for the time-of-arrival at a detector is defined for the free relativistic particle in .3 C 1/ dimensions. For each detector position there exists a subspace of detected states in the Hilbert space of solutions to the Klein¿Gordon equation. Orthogonality and completeness of the eigenfunctions of the time-of-arrival operator apply inside this subspace, opening up a standard probabilistic interpretation. c 1997 IOP Publishing Ltd-
dc.publisherInstitute of Physics Publishing-
dc.rightsopenAccess-
dc.subject[PACS] Formalism-
dc.subject[PACS] Canonical quantization-
dc.subject[PACS] Lorentz and Poincare invariance-
dc.subject[PACS] Foundations, theory of measurement, miscellaneous theories-
dc.titleTime of arrival formalism for the relativistic particle-
dc.typepreprint-
dc.identifier.doi10.1088/0305-4470/30/13/027-
dc.date.updated2014-09-29T10:37:26Z-
dc.description.versionPeer Reviewed-
dc.language.rfc3066eng-
dc.type.coarhttp://purl.org/coar/resource_type/c_816bes_ES
item.fulltextWith Fulltext-
item.openairecristypehttp://purl.org/coar/resource_type/c_816b-
item.cerifentitytypePublications-
item.openairetypepreprint-
item.grantfulltextopen-
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