2011
DOI: 10.1007/s10509-011-0626-9
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An interacting and non-interacting two-fluid scenario for dark energy in FRW universe with constant deceleration parameter

Abstract: In this paper we study the evolution of the dark energy parameter within the scope of a spatially homogeneous and isotropic FRW universe filled with barotropic fluid and dark energy. The scale factor is considered as a power law function of time which yields a constant deceleration parameter. We consider the case when the dark energy is minimally coupled to the perfect fluid as well as direct interaction with it. The cosmic jerk parameter in our derived models is consistent with the recent data of astrophysica… Show more

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Cited by 49 publications
(21 citation statements)
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References 73 publications
(44 reference statements)
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“…So a number of viable models for dark energy have been constructed. These scenarios include, quintessence [24,25], chameleon [26], K-essence [27,28], which is based on earlier work of K-inflation [29], modified gravity [30][31][32][33][34][35][36], tachyon [37] arising in string theory [38], quintessential inflation [39], Chaplygin gas as well as generalized Chaplygin gas [40][41][42][43][44][45][46], cosmological nuclear energy [47], equation of state (EoS) parameter [48][49][50][51][52][53][54][55], braneworld [56,57] and interacting dark energy models [58][59][60][61][62]. Therefore some form of dark energy whose fractional energy density is about DE = 0.70 must exist in the Universe to drive this acceleration.…”
Section: Introductionmentioning
confidence: 99%
“…So a number of viable models for dark energy have been constructed. These scenarios include, quintessence [24,25], chameleon [26], K-essence [27,28], which is based on earlier work of K-inflation [29], modified gravity [30][31][32][33][34][35][36], tachyon [37] arising in string theory [38], quintessential inflation [39], Chaplygin gas as well as generalized Chaplygin gas [40][41][42][43][44][45][46], cosmological nuclear energy [47], equation of state (EoS) parameter [48][49][50][51][52][53][54][55], braneworld [56,57] and interacting dark energy models [58][59][60][61][62]. Therefore some form of dark energy whose fractional energy density is about DE = 0.70 must exist in the Universe to drive this acceleration.…”
Section: Introductionmentioning
confidence: 99%
“…This ansatz generalized the one proposed by Amirhashchi et al [52]. In literature it is common to use a constant deceleration parameter [37,38,41,53,21,22] as it duly gives a power law for metric function or corresponding quantity. The motivation to choose such time dependent DP is behind the fact that the universe is accelerated expansion at present as observed in recent observations of Type Ia supernova [1]− [4] and CMB anisotropies [54]− [56] and decelerated expansion in the past.…”
Section: Solution Of the Field Equations And Its Physical Significancementioning
confidence: 82%
“…These observations were based on the combination of cosmological datasets coming from CMB anisotropies, luminosity distances of high redshift type Ia supernovae and galaxy clustering. Recently, Amirhashchi et al [29,30], Pradhan et al [31], Saha et al [32], Pradhan [33] and Kumar [34] have made study on FRW based dark energy model in which they considered an interacting and non-interacting two type of fluids, one for barotropic matter and other for dark energy.…”
Section: Introductionmentioning
confidence: 99%