Annotation
The Bogolyubov group is defined for $(N+1)$-dimensional systems invariant under transformations that form a Lie group, which makes it possible to carry out quantization near a time-dependent classical scalar field with allowance for conservation laws, and to solve the zero-mode problem.
© 2016 Publisher M.V.Lomonosov Moscow State University
Authors
S.Yu. Vernov, O.A. Khrustalev, M.V. Chichikina
Department of Field Theory and High-Energy Physics, Faculty of Physics, Moscow State University, Leninskie Gory, Moscow, 119992, Russia
Department of Field Theory and High-Energy Physics, Faculty of Physics, Moscow State University, Leninskie Gory, Moscow, 119992, Russia
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