Bogolyubov Quasiparticles in Constrained Systems

dc.creatorPervushin, V. N.
dc.creatorSmirichinski, V. I.
dc.date1999-02-01
dc.date1999-07-10
dc.date.accessioned2026-07-07T10:54:01Z
dc.date.available2026-07-07T10:54:01Z
dc.descriptionThe paper is devoted to the formulation of quantum field theory for an early universe in General Relativity considered as the Dirac general constrained system. The main idea is the Hamiltonian reduction of the constrained system in terms of measurable quantities of the observational cosmology: the world proper time, cosmic scale factor, and the density of matter. We define " particles" as field variables in the holomorphic representation which diagonalize the measurable density. The Bogoliubov quasiparticles are determined by diagonalization of the equations of motion (but not only of the initial Hamiltonian) to get the set of integrals of motion (or conserved quantum numbers, in quantum theory). This approach is applied to describe particle creation in the models of the early universe where the Hubble parameter goes to infinity.
dc.description13 pages, Latex
dc.identifierhttps://arxiv.org/abs/hep-th/9902013
dc.identifierhttp://arxiv.org/abs/hep-th/9902013
dc.identifierJ.Phys.A32:6191-6201,1999
dc.identifierdoi:10.1088/0305-4470/32/34/306
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/185678
dc.subjectHigh Energy Physics - Theory
dc.subjectGeneral Relativity and Quantum Cosmology
dc.titleBogolyubov Quasiparticles in Constrained Systems
dc.typetext

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