The C0C^0 Strong Cosmic Censorship conjecture for charged scalar field black holes

Let gg be the maximal globally hyperbolic development of generic regular data for the Einstein–Maxwell–Klein–Gordon system

Ricμν(g)12R(g)gμν=TμνEM+TμνKG,μFμν=q0i(ϕDνϕϕDνϕ)2,F=dA,gμνDμDνϕ=m2ϕ,\begin{aligned} \operatorname{Ric}_{\mu\nu}(g)-\frac12R(g)g_{\mu\nu}&=\mathbb{T}^{EM}_{\mu\nu}+\mathbb{T}^{KG}_{\mu\nu},\\ \nabla^\mu F_{\mu\nu}&=q_0\frac{i(\phi\overline{D_\nu\phi}-\overline\phi D_\nu\phi)}2,\qquad F=dA,\\ g^{\mu\nu}D_\mu D_\nu\phi&=m^2\phi, \end{aligned}

where D=+iq0AD=\nabla+iq_0A. C0C^0 Strong Cosmic Censorship conjecture. The maximal globally hyperbolic development is inextendible as a continuous Lorentzian manifold. The conjecture is false: dynamical charged and massive charged scalar-field black holes admit continuous extensions under the assumptions described in the paper.

Sources & referencesView supporting material

Primary source

Maxime Van de Moortel, “Mass inflation and the C^2-inextendibility of spherically symmetric charged scalar field dynamical black holes”, arXiv:2001.11156 (2020).

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