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abstract

A non-singular exact black hole solution in General Relativity is presented. The source is a non-linear electromagnetic field, which reduces to the Maxwell theory for weak field. The solution corresponds to a charged black hole with |q| \leq 2s_c m \approx 0.6 m, having metric, curvature invariants, and electric field bounded everywhere.

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fields

gr-qc 1 hep-th 1

years

2026 2

roles

background 2

polarities

background 2

representative citing papers

All $2D$ generalised dilaton theories from $d\geq 4$ gravities

hep-th · 2026-03-06 · conditional · novelty 7.0

Generic 2D Horndeski theories arise from dimensional reduction of d≥4 gravities, yielding a Birkhoff theorem for quasi-topological gravities where static spherically symmetric solutions satisfy g_tt g_rr = -1 and are determined algebraically.

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Showing 2 of 2 citing papers.

  • All $2D$ generalised dilaton theories from $d\geq 4$ gravities hep-th · 2026-03-06 · conditional · none · ref 121 · internal anchor

    Generic 2D Horndeski theories arise from dimensional reduction of d≥4 gravities, yielding a Birkhoff theorem for quasi-topological gravities where static spherically symmetric solutions satisfy g_tt g_rr = -1 and are determined algebraically.

  • $g_{tt}g_{rr} =-1$ black hole thermodynamics in extended quasi-topological gravity gr-qc · 2026-04-27 · unverdicted · none · ref 21

    A unified framework links the generating function for static black holes satisfying g_tt g_rr=-1 in extended quasi-topological gravity to thermodynamic mass and Wald entropy via an effective 2D dilaton theory.