arXiv:hep-th/0501242·v4·High Energy Physics — Theory
Hamiltonian Cosmological Perturbation Theory
B.M. Barbashov (JINR, Dubna)🇷🇺 · V.N. Pervushin (JINR, Dubna)🇷🇺 · A.F. Zakharov (NAOC, ITEP, Moscow)🇷🇺 · V.A. Zinchuk (JINR, Dubna)🇷🇺
Abstract
The Hamiltonian approach to cosmological perturbations in general relativity in finite space-time is developed, where a cosmological scale factor is identified with spatial averaging the metric determinant logarithm. This identification preserves the number of variables and leads to a cosmological perturbation theory with the scalar potential perturbations in contrast to the kinetic perturbations in the Lifshitz version which are responsible for the ``primordial power spectrum'' of CMB in the inflationary model. The Hamiltonian approach enables to explain this ``spectrum'' in terms of scale-invariant variables and to consider other topical problem of modern cosmology in the context of quantum cosmological creation of both universes and particles from the stable Bogoliubov vacuum.
Comments: 10 pages, text was changed according to the version accepted for publication in Physics Letters B