Abstract

By the application of the generalized Israel junction conditions we derive cosmological equations for the fourth-order f(R)f(R) brane gravity and study their cosmological solutions. We show that there exists a non-static solution which describes a four-dimensional de-Sitter (dS4)(dS_4) brane embedded in a five-dimensional anti-de-Sitter (AdS5)(AdS_5) bulk for a vanishing Weyl tensor contribution. On the other hand, for the case of a non-vanishing Weyl tensor contribution, there exists a static brane only. We claim that in order to get some more general non-static f(R)f(R) brane configurations, one needs to admit a dynamical matter energy-momentum tensor in the bulk rather than just a bulk cosmological constant.

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