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Harnessing S-duality inN= 4 SYM & supergravity as SL(2, Z)-averaged strings,

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

3 Pith papers citing it

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background 2

citation-polarity summary

fields

hep-th 3

years

2026 2 2025 1

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UNVERDICTED 3

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background 2

representative citing papers

M\"obius randomness in the Hartle-Hawking state

hep-th · 2025-05-05 · unverdicted · novelty 7.0

The Hartle-Hawking state for toroidal quantum cosmologies is expressed in the Langlands decomposition as a sum over zeta zeros whose near-singularity dynamics follow the Hilbert-Pólya Hamiltonian and as a Möbius average of CFT partition functions.

An observer's quantization of 3d de Sitter

hep-th · 2026-06-24 · unverdicted · novelty 6.0

Proposes an SL(2,Z) sum of Kerr-lens geometries in 3d dS gravity whose spectral density is computed via crosscap amplitudes in CLS ⊗ CLS, matching semi-classical predictions and reducing in a simple case to GΣ ⊗ GΣ on the observer worldline.

citing papers explorer

Showing 3 of 3 citing papers.

  • Positivity of the gravitational path integral implies the axionic weak gravity conjecture hep-th · 2026-05-06 · unverdicted · none · ref 74

    Positivity of gravitational path integral inner products requires non-perturbative instabilities in axion wormholes that break shift symmetry, implying a sharp axion weak gravity conjecture with precise constants.

  • M\"obius randomness in the Hartle-Hawking state hep-th · 2025-05-05 · unverdicted · none · ref 59

    The Hartle-Hawking state for toroidal quantum cosmologies is expressed in the Langlands decomposition as a sum over zeta zeros whose near-singularity dynamics follow the Hilbert-Pólya Hamiltonian and as a Möbius average of CFT partition functions.

  • An observer's quantization of 3d de Sitter hep-th · 2026-06-24 · unverdicted · none · ref 145

    Proposes an SL(2,Z) sum of Kerr-lens geometries in 3d dS gravity whose spectral density is computed via crosscap amplitudes in CLS ⊗ CLS, matching semi-classical predictions and reducing in a simple case to GΣ ⊗ GΣ on the observer worldline.