2014
DOI: 10.1007/s10714-014-1825-9
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K-essential covariant holography

Abstract: The holographic principle is applied to a flat Friedmann-Robertson-Walker space-time dominated by dark energy when this is due to the presence of a k-essence scalar field, both for dark energy and phantom scenarios. In this framework, a geometrical covariant approach permits the construction of holographic hypersurfaces. The resulting covariant preferred screens, both for phantom and non-phantom regions, are then compared with those obtained by using the holographic dark energy model with the future event hori… Show more

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“…The first UDM model with fast transition was introduced in [30] and prescribed the evolution of p. The pressure and energy density were related by a barotropic EOS, p = p(ρ) and the perturbations were adiabatic. A second UDM model with fast transition was presented in [31] and was built from a k-essence [32,33] scalar field Lagrangian (see also [34][35][36][37]). This model also prescribed p but, differently from the first one, since it is based on a scalar field the perturbations are naturally nonadiabatic [38,39], allowing for a small Jeans length even when the speed of sound is non-negligible.…”
Section: Introductionmentioning
confidence: 99%
“…The first UDM model with fast transition was introduced in [30] and prescribed the evolution of p. The pressure and energy density were related by a barotropic EOS, p = p(ρ) and the perturbations were adiabatic. A second UDM model with fast transition was presented in [31] and was built from a k-essence [32,33] scalar field Lagrangian (see also [34][35][36][37]). This model also prescribed p but, differently from the first one, since it is based on a scalar field the perturbations are naturally nonadiabatic [38,39], allowing for a small Jeans length even when the speed of sound is non-negligible.…”
Section: Introductionmentioning
confidence: 99%