Abstract:From the field equations corresponding to a four-dimensional brane embedded in the five-dimensional spacetime of the Einstein–Chern–Simons theory for gravity, we find cosmological solutions that describe an accelerated expansion for a flat universe. Apart from a quintessence-type evolution scheme, we obtain a transient phantom evolution, which is not ruled out by the current observational data. Additionally, a bouncing solution is shown. The introduction of a kinetic term in the action shows a de Sitter behavi… Show more
“…The symbol ∼ denotes 4-dimensional quantities. We will use the usual notation [8], [9] x α = (x µ , φ) ; α, β = 0, ..., 4 ; a, b = 0, ..., 4; µ, ν = 0, ..., 3 ; m, n = 0, ..., 3 ;…”
Section: Discussionmentioning
confidence: 99%
“…From (3) we can see that the Lagrangian contains the Gauss-Bonnet term L GB , the Einstein-Hilbert term L EH and a cosmological term L Λ . In fact, replacing (55) and (60) in L GB , L EH , L Λ and using εmnpq = ε mnpq4 , we obtain [8], [9] L GB = ε abcde R ab R cd e e ,…”
Section: Discussionmentioning
confidence: 99%
“…dimensional vanishing torsion conditionT m = dẽ m + ωm n ẽn = 0, (59)where f ′ = ∂f /∂φ, ωm n = ω m n and d = dx µ ∂/∂ xµ . From (58), (59) and the Cartan's second structural equation, R ab = dω ab + ω a c ω cb , we obtain the components of the 2-form curvature[8],[9] …”
We consider the five-dimensional Einstein-Gauss-Bonnet gravity, which can be obtained by means of an apropriate choice of coefficients in the five-dimensional Lanczos-Lovelock gravity theory. The Einstein-Gauss-Bonnet field equations for the Friedmann-Lemaître-Robertson-Walker metric are found as well as some of their solutions. A four-dimensional gravity action is obtained from the Gauss-Bonnet gravity using the Randall-Sundrum compactification procedure and then it is studied the implications of the compactification procedure in the cosmological solutions. The same procedure is used to obtain gravity in four dimensions from the fivedimensional AdS-Chern-Simons gravity to then study some cosmological solutions. Some aspects of the construction of the four-dimensional action gravity are considered in an Appendix.
“…The symbol ∼ denotes 4-dimensional quantities. We will use the usual notation [8], [9] x α = (x µ , φ) ; α, β = 0, ..., 4 ; a, b = 0, ..., 4; µ, ν = 0, ..., 3 ; m, n = 0, ..., 3 ;…”
Section: Discussionmentioning
confidence: 99%
“…From (3) we can see that the Lagrangian contains the Gauss-Bonnet term L GB , the Einstein-Hilbert term L EH and a cosmological term L Λ . In fact, replacing (55) and (60) in L GB , L EH , L Λ and using εmnpq = ε mnpq4 , we obtain [8], [9] L GB = ε abcde R ab R cd e e ,…”
Section: Discussionmentioning
confidence: 99%
“…dimensional vanishing torsion conditionT m = dẽ m + ωm n ẽn = 0, (59)where f ′ = ∂f /∂φ, ωm n = ω m n and d = dx µ ∂/∂ xµ . From (58), (59) and the Cartan's second structural equation, R ab = dω ab + ω a c ω cb , we obtain the components of the 2-form curvature[8],[9] …”
We consider the five-dimensional Einstein-Gauss-Bonnet gravity, which can be obtained by means of an apropriate choice of coefficients in the five-dimensional Lanczos-Lovelock gravity theory. The Einstein-Gauss-Bonnet field equations for the Friedmann-Lemaître-Robertson-Walker metric are found as well as some of their solutions. A four-dimensional gravity action is obtained from the Gauss-Bonnet gravity using the Randall-Sundrum compactification procedure and then it is studied the implications of the compactification procedure in the cosmological solutions. The same procedure is used to obtain gravity in four dimensions from the fivedimensional AdS-Chern-Simons gravity to then study some cosmological solutions. Some aspects of the construction of the four-dimensional action gravity are considered in an Appendix.
We consider the five-dimensional Einstein–Gauss–Bonnet gravity, which can be obtained by means of an appropriate choice of coefficients in the five-dimensional Lanczos–Lovelock gravity theory. The Einstein–Gauss–Bonnet field equations for the Friedmann–Lemaître–Robertson–Walker metric are found as well as some of their solutions. The hyperbolicity of the corresponding equations of motion is discussed. A four-dimensional gravity action is obtained from the Gauss–Bonnet gravity using the Randall–Sundrum compactification procedure and then it is studied the implications of the compactification procedure in the cosmological solutions. The same procedure is used to obtain gravity in four dimensions from the five-dimensional AdS–Chern–Simons gravity to then study some cosmological solutions. Some aspects of the construction of the four-dimensional action gravity, as well as a brief review of Lovelock gravity in 5D are considered in an Appendix.
“…For instance, in the framework of braneworld cosmology, in Refs. [15,16] the h-field was associated with a scalar field, exhibiting the behavior of cosmological constant (dark energy). This background could then lead to a response to the concern presented.…”
We consider a five-dimensional Einstein-Chern-Simons action which is composed of a gravitational sector and a sector of matter, where the gravitational sector is given by a Chern-Simons gravity action instead of the Einstein-Hilbert action, and where the matter sector is given by a perfect fluid. The gravitational lagrangian is obtained gauging some Liealgebras, which in turn, were obtained by S-expansion procedure of Antide Sitter and de Sitter algebras. On the cosmological plane, we discuss the field equations resulting from the Anti-de Sitter and de Sitter frameworks and we show analogies with four-dimensional cosmological schemes.
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