A Phase Space Approach to the Gravitational Arrow of Time

Abstract

We attempt to find a function that characterizes gravitational clumping and that increases monotonically as inhomogeneity increases. We choose $S=ln\Omega$ as the candidate ``gravitational entropy'' function, where $\Omega$ is the phase-space volume below the Hamiltonian H of the system under consideration. We compute $\Omega$ for transverse electromagnetic waves and for gravitational wave, radiation and density perturbations in an expanding FLRW universe. These calculations are carried out in the linear regime under the assumption that the phases of the oscillators comprising the system are random. Entropy is thus attributed to the lack of knowledge of the exact field configuration. We find that $\Omega$, and hence $ln\Omega$ behaves as required. We also carry out calculations for Bianchi IX cosmological models and find that, even in this homogeneous case, the function can be interpreted sensibly. We compare our results with Penrose's C^2 hypothesis. Because S is defined to resemble the fundamental statistical mechanics definition of entropy, we are able to recover the entropy in a variety of familiar circumstances including, evidently, black-hole entropy. The results point to the utility of the relativistic ADM Hamiltonian formalism in establishing a connection between general relativity and statistical mechanics, although fully nonlinear calculations will need to be performed to remove any doubt.

arXiv comment20 pages. To appear in Physical Review D

References in corpus (1)

• The Entropy of the Gravitational Field

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