2017
DOI: 10.1103/physrevd.95.044044
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Stability of singularity-free cosmological solutions in Hořava-Lifshitz gravity

Abstract: We study stability of singularity-free cosmological solutions with positive cosmological constant based on projectable Hořava-Lifshitz (HL) theory. In HL theory, the isotropic and homogeneous cosmological solutions with bounce can be realized if spacial curvature is non-zero. By performing perturbation analysis around non-flat Friedmann-Lemaître-Robertson-Walker (FLRW) spacetime, we derive a quadratic action and discuss the stability, i.e, ghost and tachyon-free conditions. Although the squared effective mass … Show more

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Cited by 12 publications
(18 citation statements)
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References 71 publications
(84 reference statements)
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“…In our previous paper [47], we investigated the stability of the singularity-free cosmological solutions based on the projectable HL theory. Namely, we impose following the projectability condition: (1.2) where, N is the lapse function which is one of the Arnowitt-Deser-Misner (ADM) variables.…”
Section: Introductionmentioning
confidence: 99%
“…In our previous paper [47], we investigated the stability of the singularity-free cosmological solutions based on the projectable HL theory. Namely, we impose following the projectability condition: (1.2) where, N is the lapse function which is one of the Arnowitt-Deser-Misner (ADM) variables.…”
Section: Introductionmentioning
confidence: 99%
“…Recent progresses have inspired a wave of looking for stable nonsingular bounce [13][14][15] (see also [16,17]), along the road beyond the cubic Galileon (even the Horndeski theory [18][19][20]). Moreover, the developments of scalar-tensor theory (the GLPV [21] and DHOST theory [22][23][24], the mimetic gravity [25,26]) might also be able to provide us with some chances to implement stable nonsingular cosmologies.…”
Section: Introductionmentioning
confidence: 99%
“…We conclude that, based on EFT, not only a stable nonsingular cosmological scenario may be built without getting involved in unknown physics, but also the phenomenological possibilities of its implementation are far richer than expected (see also [52,53] for the higher spatial derivative operators). …”
Section: Resultsmentioning
confidence: 99%