Nonlinear electrodynamics and stability of spherically symmetric space-times in scalar-tensor gravity
5 affiliations
- 1Rostest
- 2RUDN University
- 3National Research Nuclear University “MEPhI”
- 4Samarkand State University
- 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 -