Abstract

In this paper, we study spontaneous scalarization of asymptotically anti-de Sitter charged black holes in an Einstein–Maxwell-scalar model with a non-minimal coupling between the scalar and Maxwell fields. In this model, Reissner–Nordström-AdS (RNAdS) black holes are scalar-free black hole solutions, and may induce scalarized black holes due to the presence of a tachyonic instability of the scalar field near the event horizon. For RNAdS and scalarized black hole solutions, we investigate the domain of existence, perturbative stability against spherical perturbations and phase structure. In a micro-canonical ensemble, scalarized solutions are always thermodynamically preferred over RNAdS black holes. However, the system has much richer phase structure and phase transitions in a canonical ensemble. In particular, we report a RNAdS BH/scalarized BH/RNAdS BH reentrant phase transition, which is composed of a zeroth-order phase transition and a second-order one.

Highlights

  • We investigated spontaneous scalarization of asymptotically AdS charged black holes in an EMS model, and studied phase structure of scalarized and RNAdS black holes in a canonical ensemble

  • We focused on a non-minimal coupling function f (φ) = eαφ2, which leads to spontaneous scalarization due to the tachyonic instability of the scalar field near the event horizon

  • Scalarized black holes can be induced from RNAdS black holes on the bifurcation line, which consists of zero modes of the scalar perturbation in RNAdS black holes

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Summary

EMS Model in AdS space

We derive the equations of motion, asymptotic behavior, the Smarr relation and the Helmholtz free energy for asymptotically AdS scalarized black hole solutions in the EMS model. The action of the EMS model with a negative cosmological constant is. Where we take G = 1 for simplicity throughout this paper. In the action (1) , the scalar field φ is minimally coupled to the metric gμν and non-minimally coupled to the gauge field Aμ, Fμν = ∂μ Aν − ∂ν Aμ is the electromagnetic field strength tensor, = −3/L2 is the cosmological constant with the AdS radius L, and f (φ) is the non-minimal coupling function of the scalar and gauge fields

Equations of motion
Asymptotic behavior
Smarr relation
Free energy
Scalar perturbation around RNAdS black holes
Time-dependent perturbation around scalarized black holes
Numerical results
Scalarized black holes
Phase structure in a canonical ensemble
Discussions and conclusions
Full Text
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