Abstract
It is well known that in four dimensions, black hole solution of the Brans–Dicke–Maxwell equations is just the Reissner–Nordstrom solution with a constant scalar field. However, in n⩾4 dimensions, the solution is not yet the (n+1)-dimensional Reissner–Nordstrom solution and the scalar field is not a constant in general. In this Letter, by applying a conformal transformation to the dilaton gravity theory, we derive a class of black hole solutions in (n+1)-dimensional (n⩾4) Brans–Dicke–Maxwell theory in the background of anti-de Sitter universe. We obtain the conserved and thermodynamic quantities through the use of the Euclidean action method. We find a Smarr-type formula and perform a stability analysis in the canonical ensemble. We find that the solution is thermally stable for small α, while for large α the system has an unstable phase, where α is a coupling constant between the scalar and matter field.
Highlights
The pioneering study on scalar-tensor theories was done by Brans and Dicke several decades ago who sought to incorporate Mach’s principle into gravity [1]
The construction and analysis of the black hole solutions in anti-de Sitter (AdS) spaces is a subject of much recent interest
We found the scalar potential leading to AdS-like solutions in BDM theory
Summary
The pioneering study on scalar-tensor theories was done by Brans and Dicke several decades ago who sought to incorporate Mach’s principle into gravity [1]. According to Brans-Dicke (BD) theory the phenomenon of inertia arises from accelerations with respect to the general mass distribution of the universe. This theory can be regarded as an economic modification of general relativity which accomodates both Mach’s principle and Dirac’s large number hypothesis as new ingredients. The low-energy effective action of the string theory leads to the Einstein gravity, coupled non-minimally to a scalar dilaton field. We investigate the effect of the scalar field on the thermal stability of the solutions .
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