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Black hole destabilization via trapped quasi-normal modes

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arxiv 2504.04779 v2 pith:EHJFOGBA submitted 2025-04-07 gr-qc hep-th

classification gr-qchep-th
keywords modesblackquasi-normalholeperturbationstrappedboundarydestabilization
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In the presence of non-minimal gravitational couplings, matter field perturbations on a static black hole spacetime may develop unphysical poles in their linearized equations. Physical solutions confined in the domain between the event horizon and a pole satisfy a boundary value problem, although with boundary conditions which are different from standard quasi-normal modes. We refer to them as "trapped quasi-normal modes". Focusing on a Schwarzschild black hole in Einstein-Proca theory, we find that trapped quasi-normal modes accurately capture the behavior of perturbations under time evolution. In particular, axial-vector modes are unstable, with a growth rate that increases with multipole number. More interestingly, we uncover a new instability that affects monopole perturbations. These results confirm the existence of a novel destabilization mechanism of black holes by non-minimally coupled vector fields, with potential implications to well-studied models of modified gravity and cosmology based on vector particles.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Cosmological tensions in Proca-Nuevo theory

    hep-th 2025-11 conditional novelty 6.0 of 10

    Fitting a one-parameter vector-tensor dark energy model to CMB, BAO, and supernova data reduces the Hubble tension to about 1.5–2σ, but the preference over ΛCDM is weak and disappears once full perturbations are included.

  2. Marginally stable Schwarzschild-black-hole-non-minimally-coupled-Proca-field bound-state configurations

    gr-qc 2025-06 conditional novelty 6.0 of 10

    Near-horizon pole configurations of a non-minimally coupled Proca field around a Schwarzschild black hole have critical masses μ r_- = √3 n, with the n=1 onset mass μ_c = √3/r_-.

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