Abstract

Based on the fact that some important theories like string and M-theories predict spacetime with higher dimensions, so, in this paper, we aim to construct a theory of quintic quasitopological gravity in higher dimensions ($n\geq5$). This $(n+1)$-dimensional quintic quasitopological gravity can also lead to the most second-order linearized field equations in the spherically symmetric spacetimes. These equations can not be solved exactly and so, we obtain a new class of $(n+1)$-dimensional static solutions with numeric methods. For large values of mass parameter $m$, these solutions yield to black holes with two horizons in AdS and flat spacetimes. For dS solutions, there are two values, $m_{\rm ext}$ and $m_{\rm cri}$, which yield to a black hole with three horizons for $m_{\rm ext}<m<m_{\rm cri}$. We also calculate thermodynamic quantities for this black hole such as entropy and temperature and check the first law of thermodynamics. Finally, we analyze thermal stability of the $(n+1)$-dimensional static black hole at the horizon $r_{+}$. Unlike dS solutions, AdS ones have thermal stability for each values of $k$, but flat solutions are stable with just $k=1$.

Highlights

  • In AdS/CFT correspondence, a duality between the strongly coupled conformal field theory and anti–de Sitter gravity is established

  • For mext < m < mcri, there is a black hole with three horizons, and for m > mcri, there is a nonextreme black hole with a horizon at rþ min, where rþ min < rext

  • Quintic quasitopological gravity in five dimensions has been proposed in which its structures on asymptotically AdS spacetimes might be duals for a broad class of CFTs

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Summary

INTRODUCTION

In AdS/CFT correspondence, a duality between the strongly coupled conformal field theory and anti–de Sitter gravity is established. A new toy model for gravity in five dimensions has been introduced as quintic quasitopological gravity space [19] This gravity includes a curvature tensor of the order of R5, it leads to equations of motion which are only second order in derivatives in spherically symmetric spacetimes. We begin with an (n þ 1)-dimensional action which includes higher curvatures up to the fifth order and can produce field equations of the second order on spherically symmetric spacetimes. In the spherically symmetric spacetime (5), the quintic quasitopological Lagrangian (4) yields to a second-order field equation in higher dimensions, if we choose the coefficients ci as what we have listed in the Appendix. The obtained function fðrÞ depends on parameters r, n, m, k, L, μ 5, μ 4, μ 3, μ 2, and μ 0

THERMODYNAMICS OF THE SOLUTIONS
PHYSICAL STRUCTURE OF THE SOLUTIONS
THERMAL STABILITY
CONCLUDING REMARKS
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