Crossing the phantom divide with dissipative normal matter in the Israel–Stewart formalism

A phantom solution in the framework of the causal Israel–Stewart (IS) formalism is discussed. We assume a late time behavior of the cosmic evolution by considering only one dominant matter fluid with viscosity. In the model it is assumed a bulk viscosity of the form ξ=ξ0ρ1/2, where ρ is the energy d...

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Main Authors: Norman Cruz, Samuel Lepe
Format: Article
Language:English
Published: Elsevier 2017-04-01
Series:Physics Letters B
Online Access:http://www.sciencedirect.com/science/article/pii/S0370269317300539
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spelling doaj-497291e233d9444e913e3046aa2e44f32020-11-24T23:43:23ZengElsevierPhysics Letters B0370-26931873-24452017-04-01767C10310910.1016/j.physletb.2017.01.035Crossing the phantom divide with dissipative normal matter in the Israel–Stewart formalismNorman Cruz0Samuel Lepe1Departamento de Física, Universidad de Santiago, Casilla 307, Santiago, ChileInstituto de Física, Facultad de Ciencias, Pontificia Universidad Católica de Valparaíso, Avenida Brasil 4950, Valparaíso, ChileA phantom solution in the framework of the causal Israel–Stewart (IS) formalism is discussed. We assume a late time behavior of the cosmic evolution by considering only one dominant matter fluid with viscosity. In the model it is assumed a bulk viscosity of the form ξ=ξ0ρ1/2, where ρ is the energy density of the fluid. We evaluate and discuss the behavior of the thermodynamical parameters associated to this solution, like the temperature, rate of entropy, entropy, relaxation time, effective pressure and effective EoS. A discussion about the assumption of near equilibrium of the formalism and the accelerated expansion of the solution is presented. The solution allows to cross the phantom divide without evoking an exotic matter fluid and the effective EoS parameter is always lesser than −1 and time independent. A future singularity (big rip) occurs, but different from the Type I (big rip) solution classified in S. Nojiri, S.D. Odintsov and S. Tsujikawa (2005) [2], if we consider other thermodynamics parameters like, for example, the effective pressure in the presence of viscosity or the relaxation time.http://www.sciencedirect.com/science/article/pii/S0370269317300539
collection DOAJ
language English
format Article
sources DOAJ
author Norman Cruz
Samuel Lepe
spellingShingle Norman Cruz
Samuel Lepe
Crossing the phantom divide with dissipative normal matter in the Israel–Stewart formalism
Physics Letters B
author_facet Norman Cruz
Samuel Lepe
author_sort Norman Cruz
title Crossing the phantom divide with dissipative normal matter in the Israel–Stewart formalism
title_short Crossing the phantom divide with dissipative normal matter in the Israel–Stewart formalism
title_full Crossing the phantom divide with dissipative normal matter in the Israel–Stewart formalism
title_fullStr Crossing the phantom divide with dissipative normal matter in the Israel–Stewart formalism
title_full_unstemmed Crossing the phantom divide with dissipative normal matter in the Israel–Stewart formalism
title_sort crossing the phantom divide with dissipative normal matter in the israel–stewart formalism
publisher Elsevier
series Physics Letters B
issn 0370-2693
1873-2445
publishDate 2017-04-01
description A phantom solution in the framework of the causal Israel–Stewart (IS) formalism is discussed. We assume a late time behavior of the cosmic evolution by considering only one dominant matter fluid with viscosity. In the model it is assumed a bulk viscosity of the form ξ=ξ0ρ1/2, where ρ is the energy density of the fluid. We evaluate and discuss the behavior of the thermodynamical parameters associated to this solution, like the temperature, rate of entropy, entropy, relaxation time, effective pressure and effective EoS. A discussion about the assumption of near equilibrium of the formalism and the accelerated expansion of the solution is presented. The solution allows to cross the phantom divide without evoking an exotic matter fluid and the effective EoS parameter is always lesser than −1 and time independent. A future singularity (big rip) occurs, but different from the Type I (big rip) solution classified in S. Nojiri, S.D. Odintsov and S. Tsujikawa (2005) [2], if we consider other thermodynamics parameters like, for example, the effective pressure in the presence of viscosity or the relaxation time.
url http://www.sciencedirect.com/science/article/pii/S0370269317300539
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