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Conformal Perturbation Theory for $n$-Point Functions: Structure Constant Deformation

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arxiv 2312.13337 v1 pith:JIJPIGVA submitted 2023-12-20 hep-th

classification hep-th
keywords epsilonexactpointstructuretheoryconstantfunctionsperturbation
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

We consider conformal perturbation theory for $n$-point functions on the sphere in general 2D CFTs to first order in coupling constant. We regulate perturbation integrals using canonical hard disk excisions of size $\epsilon$ around the fixed operator insertions, and identify the full set of counter terms which are sufficient to regulate all such integrated $n$-point functions. We further explore the integrated 4-point function which computes changes to the structure constants of the theory. Using an $sl(2)$ map, the three fixed locations of operators are mapped to $0$, $1$, and $\infty$. We show that approximating the mapped excised regions to leading order in $\epsilon$ does not lead to the same perturbative shift to the structure constant as the exact in $\epsilon$ region. We explicitly compute the correction back to the exact in $\epsilon$ region of integration in terms of the CFT data. We consider the compact boson, and show that one must use the exact in $\epsilon$ region to obtain agreement with the exact results for structure constants in this theory.

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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. Covering space maps for $n$-point functions with three long twists

    hep-th 2025-07 conditional novelty 7.0 of 10

    Explicit covering-space maps for three long twists plus any number of twist-2 operators are constructed, yielding closed-form four- and five-point bare twist correlators in the ΔN=1,2 cases.

  2. Quantum chaos and pole skipping in two-dimensional conformal perturbation theory

    hep-th 2025-09 conditional novelty 6.0 of 10

    A deformed 2D CFT's stress-tensor pole-skipping point shifts at O(lambda^2); at h=1/2 the shift matches the holographic butterfly velocity.

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