Equilibrium boundary conditions, dynamic vacuum energy, and the Big Bang

dc.creatorKlinkhamer, F. R.
dc.date2008-03-03
dc.date2008-10-25
dc.date.accessioned2026-07-07T11:48:52Z
dc.date.available2026-07-07T11:48:52Z
dc.descriptionThe near-zero value of the cosmological constant Λin an equilibrium context may be due to the existence of a self-tuning relativistic vacuum variable q. Here, a cosmological nonequilibrium context is considered with a corresponding time-dependent cosmological parameter Λ(t) or vacuum energy density ρ_V(t). A specific model of a closed Friedmann-Robertson-Walker universe is presented, which is determined by equilibrium boundary conditions at one instant of time (t=t_{eq}) and a particular form of vacuum-energy dynamics (dρ_V/dt \propto ρ_M). This homogeneous and isotropic model has a standard Big Bang phase at early times (t << t_{eq}) and reproduces the main characteristics of the present universe (t=t_0 < t_{eq}).
dc.description20 pages with revtex4; v7: published version in preprint style
dc.identifierhttps://arxiv.org/abs/0803.0281
dc.identifierhttp://arxiv.org/abs/0803.0281
dc.identifierPhys.Rev.D78:083533,2008
dc.identifierdoi:10.1103/PhysRevD.78.083533
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/203031
dc.subjectGeneral Relativity and Quantum Cosmology
dc.subjectAstrophysics
dc.subjectHigh Energy Physics - Phenomenology
dc.titleEquilibrium boundary conditions, dynamic vacuum energy, and the Big Bang
dc.typetext

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