174 research outputs found

    Field equations for Lovelock gravity: An alternative route

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    We present an alternative derivation of the gravitational field equations for Lovelock gravity starting from the Newton's law, which is closer in spirit to the thermodynamic description of gravity. As a warm up exercise, we have explicitly demonstrated that projecting the Riemann curvature tensor appropriately and taking a cue from Poisson's equation, the Einstein's equations immediately follow. The above derivation naturally generalizes to Lovelock gravity theories where an appropriate curvature tensor satisfying the symmetries as well as the Bianchi derivative properties of the Riemann tensor has to be used. Interestingly, in the above derivation, the thermodynamic route to gravitational field equations, suited for null hypersurfaces, emerge quiet naturally.Comment: Invited Article; 11 pages, no figure

    Effective field equation on m-brane embedded in n-dimensional bulk of Einstein and f(R) gravity

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    We have derived effective gravitational field equations on a lower dimensional hypersurface (known as a brane), placed in a higher dimensional bulk spacetime for both Einstein and f(R)f(\mathcal{R}) gravity theories. We have started our analysis on nn-dimensional bulk from which the effective field equations on a (nβˆ’1)(n-1)-dimensional brane has been obtained by imposing Z2Z_{2} symmetry. Subsequently, we have arrived at the effective equations in (nβˆ’2)(n-2)-dimensions starting from the effective equations for (nβˆ’1)(n-1) dimensional brane. This analysis has been carried forward and is used to obtain the effective field equations in (nβˆ’m)(n-m)-dimensional brane, embedded in a nn-dimensional bulk. Having obtained the effective field equations in Einstein gravity, we have subsequently generalized the effective field equation in (nβˆ’m)(n-m)-dimensional brane which is embedded the nn-dimensional bulk spacetime endowed with f(R)f(\mathcal{R}) gravity. We have also presented applications of our results in the context of Einstein and f(R)f(\mathcal{R}) gravity. In both the cases we have discussed vacuum static spherically symmetric solutions as well as solutions in cosmological context. Implications are also discussed.Comment: v2, Revised, Accepted in EPJC, 35 pages, no figure
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