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Ay´ on-Beato, M

2 Pith papers cite this work. Polarity classification is still indexing.

2 Pith papers citing it
abstract

Black holes supported by self-interacting conformal scalar fields can be considered as renormalizably dressed since the conformal potential is nothing but the top power-counting renormalizable self-interaction in the relevant dimension. On the other hand, potentials defined by powers which are lower than the conformal one are also phenomenologically relevant since they are in fact super-renormalizable. In this work we provide a new map that allows to build black holes dressed with all the (super-)renormalizable contributions starting from known conformal seeds. We explicitly construct several new examples of these solutions in dimensions $D=3$ and $D=4$, including not only stationary configurations but also time-dependent ones.

citation-role summary

background 1

citation-polarity summary

fields

hep-th 2

years

2026 1 2025 1

verdicts

UNVERDICTED 2

roles

background 1

polarities

support 1

representative citing papers

(Super-)renormalizable hairy meronic black holes

hep-th · 2026-04-28 · unverdicted · novelty 6.0

Analytical black hole solutions are constructed in Einstein-Maxwell-Yang-Mills theory with conformally coupled scalars, generalizing MTZ and AC solutions by including non-Abelian gauge fields determined by horizon curvature.

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Showing 2 of 2 citing papers.

  • (Super-)renormalizable hairy meronic black holes hep-th · 2026-04-28 · unverdicted · none · ref 71

    Analytical black hole solutions are constructed in Einstein-Maxwell-Yang-Mills theory with conformally coupled scalars, generalizing MTZ and AC solutions by including non-Abelian gauge fields determined by horizon curvature.

  • A new rotating axionic AdS$_4$ black hole dressed with a scalar field hep-th · 2025-04-23 · unverdicted · none · ref 22 · internal anchor

    A new axionically charged rotating AdS4 black hole solution with scalar field is presented, defined by a structural function and parameters, with thermodynamics derived via Euclidean method satisfying the first law.