Poincaré-De Sitter Flow and Cosmological Meaning

preprint2012arXivOpen access

Abstract

We introduce the Poincaré-de Sitter flow with real numbers {r,s}\{r,s\} to parameterize the relativistic quadruple QPoR=[P,P2,D+,D−]M/M±/D±{\frak Q}_{PoR}=[{\cal P}, {\cal P}_2, {\cal D}_+,{\cal D}_-]_{M/M_\pm/D_\pm} for the triple of Poincaré/\dS/\AdS\ group P/D+/D−{\cal P}/{\cal D}_+/{\cal D}_- invariant special relativity. The dual Poincaré group P2{\cal P}_2-invariant degenerated Einstein manifold M±M_\pm of Λ±=±3l−2Λ_\pm=\pm3l^{-2} is for the space/time-like domain R˙±\dot R_\pm of the compact lightcone CˉO\bar C_O associated to the common space/time-like region R±R_\pm of the lightcone COC_O at common origin on Minkowski/\dS/\AdS\ spacetime M/D+/D−M/D_+/D_-. Based on the principle of relativity with two universal constants (c,l)(c, l), there are the law of inertia, coordinate time simultaneity and so on for the flow on a Poincaré-\dS\ symmetric Einstein manifold of Λs=3sl−2Λ_{s}=3{s}l^{-2}. Further, there is Robertson-Walker-like cosmos of the flow for the propertime simultaneity. The \dS\ special relativity with double [D+,P2]D+/M+[{\cal D}_+,{\cal P}_2]_{D_+/M_+} can provide a consistent kinematics for the cosmic scale physics with an upper entropy bound SR=kBπg−2,g2:=(ℓP/R)2≃10−122S_R=k_Bπg^{-2}, g^2:=(\ell_P/R)^2 \simeq 10^{-122}, for R≃(3/Λ)1/2∼13.7GlyR\simeq (3/Λ)^{1/2}\sim 13.7 Gly.

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