2010
DOI: 10.1140/epjc/s10052-010-1503-3
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Stability of the Einstein static universe in IR modified Hořava gravity

Abstract: Recently, Hořava proposed a power counting renormalizable theory for (3+1)-dimensional quantum gravity, which reduces to Einstein gravity with a non-vanishing cosmological constant in IR, but possesses improved UV behaviors. In this work, we analyze the stability of the Einstein static universe by considering linear homogeneous perturbations in the context of an IR modification of Hořava gravity, which implies a 'soft' breaking of the 'detailed balance' condition. The stability regions of the Einstein static u… Show more

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Cited by 64 publications
(51 citation statements)
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References 70 publications
(34 reference statements)
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“…In GR, this was reconsidered, and it was found that the Einstein static universe can be stable against small inhomogeneous vector and tensor perturbations as well as adiabatic scalar density perturbations if the universe contains a perfect fluid with w = c 2 s > 1/5 [25,26,31]. Of course, the stability of the Einstein static universe has also been extensively studied in many modified gravities, for example, loop quantum cosmology [32], f (R) theory [33][34][35], f (T ) theory [36,37], modified Gauss-Bonnet gravity [38,39], Brans-Dicke theory [40][41][42][43], Horava-Lifshitz theory [44][45][46], massive gravity [47,48], braneworld scenario [49][50][51], Einstein-Cartan theory [52], f (R, T ) gravity [53], hybrid metric-Palatini gravity [54] and so on [55][56][57][58][59][60][61][62]. We refer to e.g.…”
Section: Introductionmentioning
confidence: 99%
“…In GR, this was reconsidered, and it was found that the Einstein static universe can be stable against small inhomogeneous vector and tensor perturbations as well as adiabatic scalar density perturbations if the universe contains a perfect fluid with w = c 2 s > 1/5 [25,26,31]. Of course, the stability of the Einstein static universe has also been extensively studied in many modified gravities, for example, loop quantum cosmology [32], f (R) theory [33][34][35], f (T ) theory [36,37], modified Gauss-Bonnet gravity [38,39], Brans-Dicke theory [40][41][42][43], Horava-Lifshitz theory [44][45][46], massive gravity [47,48], braneworld scenario [49][50][51], Einstein-Cartan theory [52], f (R, T ) gravity [53], hybrid metric-Palatini gravity [54] and so on [55][56][57][58][59][60][61][62]. We refer to e.g.…”
Section: Introductionmentioning
confidence: 99%
“…We try to remove the initial singularity problem in the standard cosmological model by studying Einstein static Universe and its stability in the non-minimal kinetic coupled gravity theory. Actually, the stability of Einstein static state has been studied in various theories: in GR with a non-constant pressure [19], in brane world scenarios [20], in Einstein-Cartan gravity [21], in loop quantum cosmology [22], in f (R) gravity [23][24][25], in GaussBonnet gravity [26], in IR modified Hořava gravity [27], in massive gravity [28], and induced matter Brane Gravity [29]. This paper is organized as follows.…”
Section: Introductionmentioning
confidence: 99%
“…This is a strong motivation to study the ESU models along with their stability conditions in the presence of high energy corrections of GR. For instance, one can point to the works done in the context of massive gravity [54][55][56], the Hořava-Lifshitz model of gravity [57][58][59], braneworld scenarios [60][61][62][63][64], induced matter theory [65], loop quantum cosmology [66][67][68], f (R), f (T ), and f (G) gravity [69][70][71][72][73][74][75]. As discussed at the beginning of this section, gravity's rainbow or DGR is also considered as an alternative of GR with high energy corrections.…”
Section: Introductionmentioning
confidence: 99%