2003
DOI: 10.1142/s0218271803003104
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Higher Dimensional Cosmological Model in Lyra Geometry: Revisited

Abstract: In this paper we have revisited the research work of Rahman and Bera22on Kaluza–Klein cosmological model within the framework of Lyra Geometry. It has been shown that the empty universe model yields a power law relation without any assumption. The role of bulk viscosity on five-dimensional cosmological model is discussed. The physical behaviour of the models is examined in all cases.

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Cited by 21 publications
(14 citation statements)
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“…Also, in this study for (n + 2) dimensional flat FRW metric, time-like displacement field vector is defined by [49] φ i = (β(t), 0, 0, 0...0)…”
Section: Strange Quark Matter Attached To String Cloud Solutions In Lmentioning
confidence: 99%
“…Also, in this study for (n + 2) dimensional flat FRW metric, time-like displacement field vector is defined by [49] φ i = (β(t), 0, 0, 0...0)…”
Section: Strange Quark Matter Attached To String Cloud Solutions In Lmentioning
confidence: 99%
“…In recent years several authors (see Refs. [15][17] and references therein) have studied multidimensional inhomogeneous cosmological models in diferent context.…”
Section: Introductionmentioning
confidence: 99%
“…One of the motivations for introducing a decaying lambda is to reconcile the age parameter and the density parameter of the universe with recent observational data. Since spacetime was strongly curved at early times (Planck times), one naturally expects an initial huge value of the cosmological constant of the order of l −2 P = G −1 , where G is the gravitational coupling constant (Pradhan et al 2006;Singh et al 2006). As the universe expands in time, the cosmological constant should decay, thereby leading to the tiny value observed presently.…”
mentioning
confidence: 99%
“…In this short communication, we consider the (n + 2)-dimensional homogeneous universe described by the combination of the standard (1 + 3) FRW metric and n extradimensions as (Pradhan et al 2005;Singh et al 2006) ds 2 = − dt 2 + a 2 (t) dr 2 1 − kr 2 + r 2 × dθ 2 1 + sin 2 θ 1 dθ 2 2 + · · · + sin 2 θ 1 . .…”
mentioning
confidence: 99%