Journal
PHYSICS LETTERS B
Volume 674, Issue 4-5, Pages 243-249Publisher
ELSEVIER
DOI: 10.1016/j.physletb.2009.03.045
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Funding
- Research Institute for Astrophysics and Astronomy of Maragha
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We present a general solution of third order Lovelock gravity in the presence of a specific type II perfect fluid. This solution for linear equation of state, p = w(rho - 4B) contains all the known solutions of third order Lovelock gravity in the literature and some new static and radiating solutions for different values of w and B. Specially, we consider the properties of static and radiating solutions for w = 0 and w = (n - 2)(-1) with B = 0 and B not equal 0. These solutions are asymptotically flat for B = 0, while they are asymptotically (anti-)de Sitter for B not equal 0. The new static solutions for these choices of B and w present black holes with one or two horizons, extreme black holes or naked singularities provided the parameters of the solutions are chosen suitable. The static solution with w = 0 and vanishing geometrical mass (m = 0) may present a black hole with two inner and outer horizons. This is a peculiar feature of the third order Lovelock gravity, which does not occur in lower order Lovelock gravity. We also, investigate the properties of radiating solutions for these values of B and w, and compare the singularity strengths of them with the known radiating solutions of third order Lovelock gravity. (C) 2009 Elsevier B.V. All rights reserved.
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