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PreprintarXiv licencearXiv

Time-domain analysis of scalar perturbations of Kerr--Newman black holes with Chern--Simons and Maxwell couplings

Abstract

To study the onset of scalarization, we investigate linear scalar perturbations around Kerr--Newman black holes in the Einstein-Chern-Simons-Maxwell-scalar theory with quadratic Chern--Simons (CS) coupling γ (γ̂=γ/M2) and Maxwell coupling η. For this purpose, we employ hyperboloidal Rácz--Tóth evolution and a stationary axisymmetric zero-mode computation. The resulting thresholds are compared with the time-domain response at representative points. For γ̂=0, we find two asymmetric threshold branches in η, while for γ̂=η, the two branches have opposite signs and unequal magnitudes. For unequal CS and Maxwell couplings, the two real threshold branches merge as the spin or CS coupling increases.

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BibTeX
@misc{chen2026timedomain,
  title = {{Time-domain analysis of scalar perturbations of Kerr--Newman black holes with Chern--Simons and Maxwell couplings}},
  author = {Yan-Ming Chen and Hyat Huang and Meng-Yun Lai and De-Cheng Zou and Yun Soo Myung and Ming Zhang},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.06393},
  eprint = {2610.06393},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.06393},
}
RIS
TY  - UNPB
TI  - Time-domain analysis of scalar perturbations of Kerr--Newman black holes with Chern--Simons and Maxwell couplings
AU  - Yan-Ming Chen
AU  - Hyat Huang
AU  - Meng-Yun Lai
AU  - De-Cheng Zou
AU  - Yun Soo Myung
AU  - Ming Zhang
PY  - 2026
DA  - 2026/10/05
PB  - arXiv
DO  - 10.48550/arxiv.2610.06393
UR  - https://arxiv.org/abs/2610.06393
AB  - To study the onset of scalarization, we investigate linear scalar perturbations around Kerr--Newman black holes in the Einstein-Chern-Simons-Maxwell-scalar theory with quadratic Chern--Simons (CS) coupling γ (γ̂=γ/M^2) and Maxwell coupling η. For this purpose, we employ hyperboloidal Rácz--Tóth evolution and a stationary axisymmetric zero-mode computation. The resulting thresholds are compared with the time-domain response at representative points. For γ̂=0, we find two asymmetric threshold branches in η, while for γ̂=η, the two branches have opposite signs and unequal magnitudes. For unequal CS and Maxwell couplings, the two real threshold branches merge as the spin or CS coupling increases.
ER  -