Abstract

In this paper, we study the perturbations of the charged static spherically symmetric black holes in the f(R)=R−2αR model by a scalar field. We analyze the quasinormal modes spectrum, superradiant modes, and superradiant instability of the black holes. The frequency of the quasinormal modes is calculated in the frequency domain by the third-order WKB method, and in the time domain by the finite difference method. The results by the two methods are consistent and show that the black hole stabilizes quicker for larger α satisfying the horizon condition. We then analyze the superradiant modes when the massive charged scalar field is scattered by the black hole. The frequency of the superradiant wave satisfies ω∈(μ2,ωc), where μ is the mass of the scalar field, and ωc is the critical frequency of the superradiance. The amplification factor is also calculated by numerical method. Furthermore, the superradiant instability of the black hole is studied analytically, and the results show that there is no superradiant instability for such a system.

Highlights

  • The problems of dark energy (DE) and dark matter (DM) have existed for a long time, for which there are no widely recognized causes till

  • The black holes (BHs) solutions given in Equation (1) are new charged static spherically symmetric (SSS) solutions obtained from the special class of f ( R) gravity

  • The model parameter α contributes to the mass of the BH

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Summary

Introduction

The problems of dark energy (DE) and dark matter (DM) have existed for a long time, for which there are no widely recognized causes till now. The parameter α cannot be set to zero, these are new BH solutions constructed in the special class of f ( R) gravities, and cannot possibly be reduced to GR ones These BHs are asymptotically flat but with a dynamical Ricci scalar R = r12. After obtaining the BH solutions [23,24], the authors calculated some thermodynamic quantities versus the model parameter α, including the entropy, quasi-local energy, Gibbs free energy, and the Hawking temperature, etc., and providing a detailed description of the physical properties including the stability and causal structure.

The Klein–Gordon Equation
Frequency Domain
Time Domain
Superradiant Scattering
Superradiant Instability
Deficit Angle
The Frequency Condition of Superradiance
Conclusions
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