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Peer-reviewedCC BY 4.0The European Physical Journal C

Nonlinear electrodynamics and stability of spherically symmetric space-times in scalar-tensor gravity

5 affiliations
  1. 1Rostest
  2. 2RUDN University
  3. 3National Research Nuclear University “MEPhI”
  4. 4Samarkand State University
  5. 5Karshi State University

Abstract

We study linear perturbations of static, spherically symmetric solutions of scalar-tensor theories (STT) of gravity from the Bergmann-Wagoner-Nordtvedt class, sourced by nonlinear electrodynamics (NED). We obtain a general expression for the effective potential Veff V eff governing the perturbation dynamics for theories with arbitrary scalar-electromagnetic interaction of the form L(ψ , F) L ( ψ , F ) , where ψ ψ is a scalar field and F = Fμ ν Fμ ν F = F μ ν F μ ν the electromagnetic invariant. This consideration includes, in particular, arbitrary scalar self-interaction potentials and scalar fields that can be phantom in some regions of space-time (the so-called trapped ghosts). Only radial (monopole) perturbations are considered here as the most likely ones to cause an instability. It is shown, in particular, that if NED has a correct Maxwell weak field limit, the zero charge limit of Veff V eff does not contain any trace of NED, and the perturbation dynamics is the same as for vacuum STT solutions. The previously obtained stability results for STT-Maxwell solutions are shown to be extended without change to STT-NED solutions with equal electric and magnetic charges, implying F =0 F = 0 . As an example of a solution with Fnot ≡ 0 F ≢ 0 , we consider a system with a massless scalar and truncated Born-Infeld NED, both minimally coupled to gravity, in GR, and show that almost all results previously obtained for F=0 F = 0 are qualitatively preserved.

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BibTeX
@article{bronnikov2026nonlinear,
  title = {{Nonlinear electrodynamics and stability of spherically symmetric space-times in scalar-tensor gravity}},
  author = {Kirill A. Bronnikov and Rustam Ibadov and Feruza Y. Shaymanova and Najibullokhon M. Shukurullokhon},
  journal = {The European Physical Journal C},
  year = {2026},
  month = oct,
  doi = {10.1140/epjc/s10052-026-16469-3},
  url = {https://link.springer.com/article/10.1140/epjc/s10052-026-16469-3},
  note = {CC BY 4.0},
}
RIS
TY  - JOUR
TI  - Nonlinear electrodynamics and stability of spherically symmetric space-times in scalar-tensor gravity
AU  - Kirill A. Bronnikov
AU  - Rustam Ibadov
AU  - Feruza Y. Shaymanova
AU  - Najibullokhon M. Shukurullokhon
PY  - 2026
DA  - 2026/10/20
JO  - The European Physical Journal C
DO  - 10.1140/epjc/s10052-026-16469-3
UR  - https://link.springer.com/article/10.1140/epjc/s10052-026-16469-3
AB  - We study linear perturbations of static, spherically symmetric solutions of scalar-tensor theories (STT) of gravity from the Bergmann-Wagoner-Nordtvedt class, sourced by nonlinear electrodynamics (NED). We obtain a general expression for the effective potential V_eff V eff governing the perturbation dynamics for theories with arbitrary scalar-electromagnetic interaction of the form L(ψ , F) L ( ψ , F ) , where ψ ψ is a scalar field and F = F_μ ν F^μ ν  F = F μ ν F μ ν the electromagnetic invariant. This consideration includes, in particular, arbitrary scalar self-interaction potentials and scalar fields that can be phantom in some regions of space-time (the so-called trapped ghosts). Only radial (monopole) perturbations are considered here as the most likely ones to cause an instability. It is shown, in particular, that if NED has a correct Maxwell weak field limit, the zero charge limit of V_eff V eff does not contain any trace of NED, and the perturbation dynamics is the same as for vacuum STT solutions. The previously obtained stability results for STT-Maxwell solutions are shown to be extended without change to STT-NED solutions with equal electric and magnetic charges, implying F =0 F = 0 . As an example of a solution with Fnot ≡ 0 F ≢ 0 , we consider a system with a massless scalar and truncated Born-Infeld NED, both minimally coupled to gravity, in GR, and show that almost all results previously obtained for F=0 F = 0 are qualitatively preserved.
SN  - 1434-6044
SN  - 1434-6052
ER  -