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Quasinormal modes of (Anti-)de Sitter black holes in the 1/D expansion,

3 Pith papers cite this work. Polarity classification is still indexing.

3 Pith papers citing it

citation-role summary

background 1

citation-polarity summary

fields

gr-qc 2 hep-th 1

years

2026 3

verdicts

UNVERDICTED 3

roles

background 1

polarities

background 1

representative citing papers

Black Hole Ringdown Nonlinearities in the Large-D Limit

gr-qc · 2026-06-22 · unverdicted · novelty 6.0

In the large-D limit, analytic third-order nonlinear corrections to quasinormal modes improve ringdown modeling accuracy by several orders of magnitude for head-on black hole collisions.

A fluid dual to charged large D membrane paradigm

hep-th · 2026-05-15 · unverdicted · novelty 6.0

The leading-order dynamics of charged large D membranes dual to asymptotically flat black holes correspond to a relativistic charged fluid localized on the membrane, with transport coefficients extracted in Eckart and Landau frames showing negative thermal conductivity and heat capacity for enforced

citing papers explorer

Showing 3 of 3 citing papers.

  • Black Hole Ringdown Nonlinearities in the Large-D Limit gr-qc · 2026-06-22 · unverdicted · none · ref 51

    In the large-D limit, analytic third-order nonlinear corrections to quasinormal modes improve ringdown modeling accuracy by several orders of magnitude for head-on black hole collisions.

  • A fluid dual to charged large D membrane paradigm hep-th · 2026-05-15 · unverdicted · none · ref 3

    The leading-order dynamics of charged large D membranes dual to asymptotically flat black holes correspond to a relativistic charged fluid localized on the membrane, with transport coefficients extracted in Eckart and Landau frames showing negative thermal conductivity and heat capacity for enforced

  • Two types of quasinormal modes of Casadio-Fabbri-Mazzacurati brane-world black holes gr-qc · 2026-02-11 · unverdicted · none · ref 18

    Quasinormal modes of massive scalars in CFM brane-world black holes split into two types, with modes disappearing at critical masses where real or imaginary frequency parts reach zero.