Scalarized charged black holes with scalar mass term

preprint2019arXivOpen access

Abstract

We study the scalarized charged black holes in the Einstein-Maxwell-Scalar (EMS) theory with scalar mass term. In this work, the scalar mass term is chosen to be mϕ2=α/βm^2_ϕ=α/β, where αα is a coupling parameter and ββ is a mass-like parameter. It turns out that any scalarized charged black holes are not allowed for the case of β≤4.4β\le 4.4 with q=0.7(M=0.5,Q=0.35)q=0.7(M=0.5,Q=0.35) because this case implies the stable Reissner-Nodström (RN) black holes. In the massless limit of β→∞β\to \infty, one recovers the case of the EMS theory. We note that the unstable RN black hole implies the appearance of scalarized charged black holes. The other unstable case of β>4.4β>4.4 with q=0.7q=0.7 allows us to obtain the n=0,1,2,⋯n=0,1,2,\cdots scalarized charged black holes for α(β)≥αth(β)α(β)\ge α_{\rm th}(β) where αth(β)α_{\rm th}(β) represents the threshold of instability for the RN black hole. Furthermore, it is shown that the n=0n=0 black hole is stable against radial perturbations, while the n=1n=1 black hole is unstable. This stability result is independent of the mass parameter ββ.

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