Hamiltonian General Relativity in Finite Space and Cosmological Potential Perturbations

Details Hamiltonian General Relativity in Finite Space and Cosmological Potential Perturbations Hamiltonian General Relativity in Finite Space and Cosmological Potential Perturbations

2005-11-30

arxiv.org/abs/astro-ph/0511824v2

Int.J.Mod.Phys.A21:5957-5990,2006

Astronomy and Astrophysics

Astrophysics

30 pages, 3 figures

Scientific paper

10.1142/S0217751X06034252

The Hamiltonian formulation of general relativity (GR) is considered in finite space-time and a specific frame of reference given by the diffeo-invariant components of the Fock simplex in terms of the Dirac -- ADM variables. The evolution parameter and energy invariant with respect to the time-coordinate transformations are constructed by the separation of the cosmological scale factor and its identification with the spatial averaging of the metric determinant, so that the dimension of the kinemetric group of diffeomorphisms coincides with the dimension of a set of variables whose velocities are removed by the Gauss-type constraints in accordance with the second N\"other theorem. This coincidence allows us to solve the energy constraint, fulfil Dirac's Hamiltonian reduction, and to describe the potential perturbations in terms of the Lichnerowicz scale-invariant variables distinguished by the absence of the time derivatives of the spatial metric determinant. It was shown that the Hamiltonian version of the cosmological perturbation theory acquires attributes of the theory of superfluid liquid, and it leads to the generalization of the Schwarzschild solution. The astrophysical application of this approach to GR is considered under supposition that the Dirac -- ADM Hamiltonian frame is identified with that of the Cosmic Microwave Background radiation distinguished by its dipole component in the frame of an Earth observer.

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