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Quadratic Fermion Interaction Hamiltonian

dc.contributor.authorGidas, Basilisen_US
dc.date.accessioned2010-05-06T22:19:31Z
dc.date.available2010-05-06T22:19:31Z
dc.date.issued1971-07en_US
dc.identifier.citationGidas, Basilis (1971). "Quadratic Fermion Interaction Hamiltonian." Journal of Mathematical Physics 12(7): 1414-1419. <http://hdl.handle.net/2027.42/70542>en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/70542
dc.description.abstractThe interaction Hamiltonian λ ∫ :(0)(x)ψ(0)(x):g(x)dsx,g(x) ∊ S(Rs)λ∫:ψ̄(0)(x)ψ(0)(x):g(x)dsx,g(x)∊S(Rs) is studied. An ultraviolet cutoff is introduced. We remove this cutoff, and take the limit g → 1 in S(Rs)S(Rs), by working with the Heisenberg fields. The limiting fields are well defined on the Fock space associated with the bare mass m0. In the limit we get a new representation of the canonical anticommutation relations which is given by a (generalized) Bogoliubov transformation. The new representation is not always unitarily equivalent to the bare mass Fock representations.en_US
dc.format.extent3102 bytes
dc.format.extent332853 bytes
dc.format.mimetypetext/plain
dc.format.mimetypeapplication/pdf
dc.publisherThe American Institute of Physicsen_US
dc.rights© The American Institute of Physicsen_US
dc.titleQuadratic Fermion Interaction Hamiltonianen_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumPhysics Department, University of Michigan, Ann Arbor, Michigan 48104en_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/70542/2/JMAPAQ-12-7-1414-1.pdf
dc.identifier.doi10.1063/1.1665749en_US
dc.identifier.sourceJournal of Mathematical Physicsen_US
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dc.owningcollnamePhysics, Department of


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