2016
DOI: 10.1007/s10474-016-0612-3
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On weakly cyclic Z symmetric spacetimes

Abstract: The object of the present paper is to study weakly cyclic Z symmetric spacetimes. At first we prove that a weakly cyclic Z symmetric spacetime is a quasi Einstein spacetime. Then we study (W CZS) 4 spacetimes satisfying the condition div C = 0. Next we consider conformally flat (W CZS) 4 spacetimes. Finally, we characterise dust fluid and viscous fluid (W CZS) 4 spacetimes.

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Cited by 7 publications
(4 citation statements)
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“…The findings presented in this study hold great significance for geometers in their future research endeavors. For example, these results can be applied to various types of space-times, such as Z recurrent space-times [49], almost pseudo Z symmetric space-times [11], weakly Z symmetric space-times [66], and weakly cyclic Z symmetric space-times [47,48].…”
Section: Condition Conclusionmentioning
confidence: 99%
“…The findings presented in this study hold great significance for geometers in their future research endeavors. For example, these results can be applied to various types of space-times, such as Z recurrent space-times [49], almost pseudo Z symmetric space-times [11], weakly Z symmetric space-times [66], and weakly cyclic Z symmetric space-times [47,48].…”
Section: Condition Conclusionmentioning
confidence: 99%
“…This manifold has received a great deal of attention and is studied in considerable detail by many authors [26][27][28][29][30][31][32][33]. Motivated by the above studies, in the present, we examine the properties of the Z-tensor of a Riemannian manifold admitting the projective curvature tensor.…”
Section: The Z-tensor On a Riemannian Manifoldmentioning
confidence: 99%
“…By virtue of ( 37) and (41) and the fact that Z-symmetric tensor is covariantly constant, the relation (38) reduces to 4k(∇ U p)φ(Y)φ(V) + k(∇ U p)g(Y, V) = 0, which by taking Y = V = ξ and using (30) leads to ∇ U p = 0, i.e., the isotropic pressure p is constant. Thus from (37), we lead to ∇ U σ = 0, i.e., the energy density is constant. This completes the proof.…”
Section: (Zs) 4 Spacetimes Admitting Schouten Tensormentioning
confidence: 99%