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

3 Pith papers citing it

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hep-th 3

years

2026 2 2025 1

representative citing papers

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 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.

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Showing 3 of 3 citing papers.

  • The analytic bootstrap at finite temperature hep-th · 2025-06-06 · conditional · none · ref 61

    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 conformal partial waves from flat-space and defect CFT hep-th · 2026-05-26 · unverdicted · none · ref 39

    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 · none · ref 17

    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.