2021
DOI: 10.48550/arxiv.2106.07396
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Exact Solutions in Higher-Dimensional Lovelock and $AdS_5$ Chern-Simons Gravity

Francesco Bajardi,
Daniele Vernieri,
Salvatore Capozziello

Abstract: Lovelock gravity in D-dimensional space-times is considered adopting Cartan's structure equations. In this context, we find out exact solutions in cosmological and spherically symmetric backgrounds. In the latter case, we also derive horizons and the corresponding Bekenstein-Hawking entropies. Moreover, we focus on the topological Chern-Simons theory, providing exact solutions in 5 dimensions. Specifically, it is possible to show that Anti-de Sitter invariant Chern-Simons gravity can be framed within Lovelock-… Show more

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Cited by 3 publications
(5 citation statements)
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“…Here we would like to mention that in four dimensional spacetime, a special case of Lanczos-Lovelock theory, namely the Gauss-Bonnet (GB) theory becomes a total surface term and thus has no contributions in the field equations. The scenario however becomes different in higher dimensional spacetime where the GB term affects the field equations non-trivially [89]. Coming back to our present model, i.e the Chern-Simons corrected F(R) model in four dimensional FRW spacetime, the Chern-Simons term shows no contributions in the background Friedmann equations, and thus the background evolution is entirely controlled by the vacuum F(R) term (see Eq.…”
Section: Essential Features Of Chern-simons F(r) Gravitymentioning
confidence: 58%
See 2 more Smart Citations
“…Here we would like to mention that in four dimensional spacetime, a special case of Lanczos-Lovelock theory, namely the Gauss-Bonnet (GB) theory becomes a total surface term and thus has no contributions in the field equations. The scenario however becomes different in higher dimensional spacetime where the GB term affects the field equations non-trivially [89]. Coming back to our present model, i.e the Chern-Simons corrected F(R) model in four dimensional FRW spacetime, the Chern-Simons term shows no contributions in the background Friedmann equations, and thus the background evolution is entirely controlled by the vacuum F(R) term (see Eq.…”
Section: Essential Features Of Chern-simons F(r) Gravitymentioning
confidence: 58%
“…( 5)). This is in contrast to [89] where the authors considered an AdS invariant Chern-Simons Lagrangian in f ive dimensional spacetime, which can be recovered from the Lovelock theory, and found the corresponding cosmological as well as spherically symmetric solutions. On contrary, in our present scenario (which is a four dimensional spacetime model), the effective energy density and pressure arises from the higher curvature F(R) degrees of freedom drive the background evolution.…”
Section: Essential Features Of Chern-simons F(r) Gravitymentioning
confidence: 69%
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“…There is quite some interest in higher Chern-Simons theories in theoretical physics (a sample selection spanning over three decades: the seminal and well known [9], [10], the excellent review [31]; see also the recent [4]) and it should be, thus, interesting to investigate the consequences of our findings.…”
Section: Introductionmentioning
confidence: 99%
“…Due to the AdS/CFT 1 correspondence, the above Lagrangian is mainly considered in five dimensions, where cosmological and spherically symmetric solutions can be analytically found [43][44][45][46][47][48][49][50][51][52][53].…”
Section: Introductionmentioning
confidence: 99%

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