Collective classical motion on hyperbolic spacetimes of any dimensions
arXiv:1802.01959 · doi:10.1142/S0217732319501657
Abstract
The geodesics equations on de Sitter and anti-de Sitter spacetimes of any dimensions, are the starting point for deriving the general form of the Boltzmann equation in terms of conserved quantities. The simple equation for the non-equilibrium Marle and Anderson-Witting models are derived and the distributions of the Boltzmann-Marle model on these manifolds are written down first in terms of conserved quantities and then as functions of canonical variables.
13 pages, no figures
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