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Euclidean Fermi fields with a hermitean Feynman-Kac-Nelson formula. I

dc.contributor.authorWilliams, David N.en_US
dc.date.accessioned2006-09-11T17:52:13Z
dc.date.available2006-09-11T17:52:13Z
dc.date.issued1974-03en_US
dc.identifier.citationWilliams, David N.; (1974). "Euclidean Fermi fields with a hermitean Feynman-Kac-Nelson formula. I." Communications in Mathematical Physics 38(1): 65-80. <http://hdl.handle.net/2027.42/46510>en_US
dc.identifier.issn1432-0916en_US
dc.identifier.issn0010-3616en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/46510
dc.description.abstractWe construct free, Euclidean, spin one-half, quantum fields with the following properties: (i) CAR; (ii) Symanzik positivity; (iii) Osterwalder-Schrader positivity; (iv) no doubling of particle or spin states. They admit the recovery of the relativistic Dirac field by the Osterwalder-Schrader technique. We then formally parametrize interacting theories by a natural class of Hermitean, Euclidean actions, and obtain a simple, Hermitean, Feynman-Kac-Nelson formula. The interacting theory formally obeys all the properties (i)–(iv), and admits the reconstruction of a physical Hilbert space, including a Hermitean, contraction semigroup for the Wick rotated time evolution. We propose a system of axioms for the interacting theory.en_US
dc.format.extent790340 bytes
dc.format.extent3115 bytes
dc.format.mimetypeapplication/pdf
dc.format.mimetypetext/plain
dc.language.isoen_US
dc.publisherSpringer-Verlagen_US
dc.subject.otherQuantum Computing, Information and Physicsen_US
dc.subject.otherStatistical Physicsen_US
dc.subject.otherMathematical and Computational Physicsen_US
dc.subject.otherQuantum Physicsen_US
dc.subject.otherPhysicsen_US
dc.subject.otherNonlinear Dynamics, Complex Systems, Chaos, Neural Networksen_US
dc.subject.otherRelativity and Cosmologyen_US
dc.titleEuclidean Fermi fields with a hermitean Feynman-Kac-Nelson formula. Ien_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbsecondlevelMathematicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumInstitut für Theoretische Physik, Freie Universität Berlin, Berlin; The Harrison M. Randall Laboratory of Physics, The University of Michigan, 48104, Ann Arbor, USAen_US
dc.contributor.affiliationumcampusAnn Arboren_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/46510/1/220_2005_Article_BF01651549.pdfen_US
dc.identifier.doihttp://dx.doi.org/10.1007/BF01651549en_US
dc.identifier.sourceCommunications in Mathematical Physicsen_US
dc.owningcollnameInterdisciplinary and Peer-Reviewed


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