Derives EFT corrections to deflection angle, photon sphere radius, critical impact parameter, and strong lensing coefficients for Reissner-Nordström black holes in weak and strong deflection regimes.
Photon Surfaces in Higher-Curvature Gravity: Implications for Quasinormal Modes and Gravitational Lensing
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abstract
Effective field theory (EFT) provides a systematic framework to describe possible deviations from general relativity through higher-curvature corrections to the gravitational action, capturing low-energy effects of an underlying fundamental theory. In this work, we investigate quasinormal modes (QNMs) and both weak and strong gravitational lensing in static, spherically symmetric spacetimes, focusing on the behavior of null geodesics near the photon sphere. Adopting the strong deflection limit formalism developed by Bozza, we derive the logarithmic divergence structure of the deflection angle and explicitly separate the divergent and regular contributions. Within a simplified setup with $2M=1$, we analyze how deviations from general relativity, parametrized in an EFT framework, modify key observables such as the photon sphere radius, the critical impact parameter, and the coefficients governing the strong deflection expansion. We show that these quantities encode direct information about higher-curvature corrections to the gravitational action. Our results demonstrate that strong-field observables provide a sensitive probe of EFT corrections, and that precision measurements of gravitational lensing and QNM spectra could place constraints on EFT couplings beyond general relativity, offering a novel observational window into quantum gravity-inspired effects.
fields
gr-qc 1years
2026 1verdicts
UNVERDICTED 1representative citing papers
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Probing Effective Field Theory Corrections with Quasinormal Modes and Gravitational Lensing in Reissner-Nordstr\"om Black Holes
Derives EFT corrections to deflection angle, photon sphere radius, critical impact parameter, and strong lensing coefficients for Reissner-Nordström black holes in weak and strong deflection regimes.