2015
DOI: 10.1007/s10509-015-2494-1
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Bianchi type-III models with anisotropic dark energy in Brans–Dicke–Rastall theory

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Cited by 10 publications
(8 citation statements)
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“…Therefore, because λ is constant and the R(4κ λ − 1) = κ T condition applies to all spacetimes and energy-momentum sources, the κ λ = 1 4 case is not allowed [23]. More studies on the various aspects of this theory can be found in [74,[77][78][79][80][81][82][83][84][85][86][87][88][89][90].…”
Section: A Brief Review On the Rastall Theorymentioning
confidence: 99%
“…Therefore, because λ is constant and the R(4κ λ − 1) = κ T condition applies to all spacetimes and energy-momentum sources, the κ λ = 1 4 case is not allowed [23]. More studies on the various aspects of this theory can be found in [74,[77][78][79][80][81][82][83][84][85][86][87][88][89][90].…”
Section: A Brief Review On the Rastall Theorymentioning
confidence: 99%
“…(4), the functionality of S R A with respect to the horizon area (A) is the same as that of the Bekenstein-Hawking entropy (S R A ∼ A) meaning that S R A may be considered as a special case of Eq. (22). More detailed studies on gravitational and cosmological implications of Tsallis entropy (22) can be found in Refs.…”
Section: Rényi Entropy and Friedmann Equationsmentioning
confidence: 99%
“…(22). More detailed studies on gravitational and cosmological implications of Tsallis entropy (22) can be found in Refs. [63][64][65][66][67][68][69][70][71][72] and references therein.…”
Section: Rényi Entropy and Friedmann Equationsmentioning
confidence: 99%
“…More studies on this theory can also be found in Refs. [37][38][39][40][41][42][43][44][45][46][47][48][49][50][51].…”
Section: Introductionmentioning
confidence: 99%