Please use this identifier to cite or link to this item: http://hdl.handle.net/2289/1279
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dc.contributor.authorNityananda, R.-
dc.contributor.authorSamuel, J.-
dc.date.accessioned2006-05-18T11:20:31Z-
dc.date.available2006-05-18T11:20:31Z-
dc.date.issued1992-05-15-
dc.identifier.citationPhysical Review D, 1992, Vol.45, 3862-3864en
dc.identifier.issn1550-7998 (print)-
dc.identifier.urihttp://hdl.handle.net/2289/1279-
dc.description.abstractKovner has observed that Fermat's principle can be used to describe the motion of light rays in arbitrary gravitational fields, not just stationary ones. We give a simple demonstration of this fact.en
dc.format.extent493392 bytes-
dc.format.mimetypeapplication/pdf-
dc.language.isoenen
dc.publisherThe American Physical Societyen
dc.relation.urihttp://link.aps.org/abstract/PRD/v45/p3862en
dc.rights(1992) by the American Physical Societyen
dc.titleFermat's principle in general relativityen
dc.typeArticleen
Appears in Collections:Research Papers (TP)

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