Please use this identifier to cite or link to this item: http://hdl.handle.net/2289/1239
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dc.contributor.authorIyer, B.R.-
dc.date.accessioned2006-05-16T09:02:16Z-
dc.date.available2006-05-16T09:02:16Z-
dc.date.issued1982-10-15-
dc.identifier.citationPhysical Review D, 1982, Vol.26, 1900-1905en
dc.identifier.issn1550-7998-
dc.identifier.urihttp://hdl.handle.net/2289/1239-
dc.description.abstractThe Dirac field in Minkowski spacetime is quantized in a rotating coordinate system. In contrast to the scalar case, the natural procedure of defining particles via the Killing vector of the rotating observer yields a canonical quantization scheme. This scheme is inequivalent to the usual Minkowski quantization, and in contrast to the scalar case the rotating observer sees in the inertial vacuum a (nonthermal) spectrum of particles and antiparticles.en
dc.format.extent600992 bytes-
dc.format.mimetypeapplication/pdf-
dc.language.isoenen
dc.publisherThe American Physical Societyen
dc.relation.urihttp://link.aps.org/abstract/PRD/v26/p1900en
dc.rights(1982) by the American Physical Societyen
dc.titleDirac field theory in rotating coordinatesen
dc.typeArticleen
Appears in Collections:Research Papers (TP)

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