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

7 Pith papers citing it

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hep-th 7

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2026 6 2025 1

representative citing papers

CFTs on Squashed Spheres and the Thermal Effective Action

hep-th · 2026-06-29 · unverdicted · novelty 7.0

Derives universal quadratic response of 3D CFT free energy to S^3 squashing proportional to c_T and constructs thermal effective action for high-T Seifert manifolds with explicit Wilson coefficients.

The analytic bootstrap at finite temperature

hep-th · 2025-06-06 · conditional · novelty 7.0

Thermal two-point functions of scalar CFT operators at zero spatial separation are reconstructed from their discontinuities via Hurwitz zeta kernels, with OPE coefficients as the only dynamical input.

Thermal effective action for the $O(N)$ vector model

hep-th · 2026-06-03 · unverdicted · novelty 6.0

Leading coefficients of the thermal effective action for the large-N critical O(N) vector model in 3D with twist are computed via twisted partition function on S2 and path-integral methods, yielding consistent results.

Thermal conformal partial waves from flat-space and defect CFT

hep-th · 2026-05-26 · unverdicted · novelty 6.0

Establishes correspondence between flat, thermal, and defect conformal partial waves via shadow formalism, obtaining thermal blocks from flat four-point and defect two-point functions and reducing the Casimir equation diagonally.

A thermal representation for conformal ladder integrals

hep-th · 2026-06-29 · unverdicted · novelty 3.0

Conformal ladder integrals are represented via thermal free energies of massive scalars, obey a second-order differential equation in even dimensions at any loop order, and admit an all-loop resummation for arbitrary D.

citing papers explorer

Showing 7 of 7 citing papers.

  • CFTs on Squashed Spheres and the Thermal Effective Action hep-th · 2026-06-29 · unverdicted · none · ref 27

    Derives universal quadratic response of 3D CFT free energy to S^3 squashing proportional to c_T and constructs thermal effective action for high-T Seifert manifolds with explicit Wilson coefficients.

  • Thermal One-point Functions and Asymptotic CFT Data: QFT in AdS hep-th · 2026-06-15 · unverdicted · none · ref 56

    Thermal inversion formulas produce asymptotically accurate CFT data for heavy operators that remains reliable at intermediate dimensions and survives first-order bulk interactions.

  • The analytic bootstrap at finite temperature hep-th · 2025-06-06 · conditional · none · ref 26

    Thermal two-point functions of scalar CFT operators at zero spatial separation are reconstructed from their discontinuities via Hurwitz zeta kernels, with OPE coefficients as the only dynamical input.

  • Thermal effective action for the $O(N)$ vector model hep-th · 2026-06-03 · unverdicted · none · ref 27

    Leading coefficients of the thermal effective action for the large-N critical O(N) vector model in 3D with twist are computed via twisted partition function on S2 and path-integral methods, yielding consistent results.

  • Thermal conformal partial waves from flat-space and defect CFT hep-th · 2026-05-26 · unverdicted · none · ref 18

    Establishes correspondence between flat, thermal, and defect conformal partial waves via shadow formalism, obtaining thermal blocks from flat four-point and defect two-point functions and reducing the Casimir equation diagonally.

  • Semi-universality of conformal higher-derivative and conformal higher-spin fields hep-th · 2026-06-07 · unverdicted · none · ref 27

    Thermal partition functions of conformal higher-derivative and higher-spin fields develop universal poles in (1-|ω_i|) in the semi-universal limit, with residues sensitive to negative-twist states, verified via mode sums and operator counting and reproduced from AdS5.

  • A thermal representation for conformal ladder integrals hep-th · 2026-06-29 · unverdicted · none · ref 34

    Conformal ladder integrals are represented via thermal free energies of massive scalars, obey a second-order differential equation in even dimensions at any loop order, and admit an all-loop resummation for arbitrary D.