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PreprintCC BY-NC-SA 4.0arXiv

Extremal Scalarization of Charged Black Holes: Miransky Scaling across Reissner-Nordström Extremality

Abstract

We study spontaneous scalarization near and at extremality in Einstein-Maxwell-scalar theory. As Reissner-Nordström (RN) extremality is approached from below, the nonextremal scalarization existence curves collapse toward a common critical threshold αc=1/4 given by the Breitenlohner-Freedman bound for the near-horizon throat (AdS2× S2) of its extremal black hole. For a polynomial coupling, we construct extremal black holes with nonconstant scalar hair, satisfying M2+Qs2=Q2, which places them in the overcharged region Q/M>1 beyond the RN bound. A common near-region phase mechanism predicts accumulation toward the RN extremality from both sides, yielding Miransky-type scaling. In the extremal sector, the logarithmic phase interval doubles, halving the exponent which denotes the geometric spacing of successive node scales.

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BibTeX
@misc{guo2026extremal,
  title = {{Extremal Scalarization of Charged Black Holes: Miransky Scaling across Reissner-Nordström Extremality}},
  author = {Hong Guo and Yun Soo Myung and Lijing Shao},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.20040},
  eprint = {2609.20040},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.20040},
  note = {CC BY-NC-SA 4.0},
}
RIS
TY  - UNPB
TI  - Extremal Scalarization of Charged Black Holes: Miransky Scaling across Reissner-Nordström Extremality
AU  - Hong Guo
AU  - Yun Soo Myung
AU  - Lijing Shao
PY  - 2026
DA  - 2026/09/17
PB  - arXiv
DO  - 10.48550/arxiv.2609.20040
UR  - https://arxiv.org/abs/2609.20040
AB  - We study spontaneous scalarization near and at extremality in Einstein-Maxwell-scalar theory. As Reissner-Nordström (RN) extremality is approached from below, the nonextremal scalarization existence curves collapse toward a common critical threshold α_c=1/4 given by the Breitenlohner-Freedman bound for the near-horizon throat (AdS_2× S^2) of its extremal black hole. For a polynomial coupling, we construct extremal black holes with nonconstant scalar hair, satisfying M^2+Q_s^2=Q^2, which places them in the overcharged region Q/M>1 beyond the RN bound. A common near-region phase mechanism predicts accumulation toward the RN extremality from both sides, yielding Miransky-type scaling. In the extremal sector, the logarithmic phase interval doubles, halving the exponent which denotes the geometric spacing of successive node scales.
ER  -