Cosmic acceleration from first principles
arXiv:2106.16014 · doi:10.1016/j.dark.2021.100892
Abstract
General relativistic entropic acceleration theory may explain the present cosmic acceleration from first principles without the need of introducing a cosmological constant. Following the covariant formulation of non-equilibrium phenomena in the context of a homogeneous and isotropic Friedmann-Lemaitre-Robertson-Walker (FLRW) metric, we find that the growth of entropy associated with the causal horizon of our universe (inside a finite bubble in eternal inflation) induces an acceleration that is essentially indistinguishable from that of CDM, except for a slightly larger present rate of expansion compared to what would be expected from the CMB in CDM, possibly solving the so-called tension. The matter content of the universe is unchanged and the coincidence problem is resolved since it is the growth of the causal horizon of matter that introduces this new relativistic entropic force. The cosmological constant is made unnecessary and the future hypersurface is Minkowsky rather than de Sitter.
arXiv comment6 pages, 5 figures. Comments added. Matches version accepted by PDU
References in corpus (7)
- The World as a Hologram
- Cosmology and Fundamental Physics with the Euclid Satellite
- A Covariant Entropy Conjecture
- The Expansion of the Universe is Faster than Expected
- More out of less: an excess integrated Sachs-Wolfe signal from supervoids mapped out by the Dark Energy Survey
- The Cosmological Constant as a Zero Action Boundary
- Covariant formulation of non-equilibrium thermodynamics in General Relativity
Cited by in corpus (6)
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- Qualitative analysis for viscous cosmologies in a non linear regime of the Israel-Stewart formalism
- Holography and matter creation revisited
- Thermodynamics of an universe with Decaying Cold Dark Matter
- Exploring the cosmological degeneracy between decaying dark matter model and viscous CDM