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CFT correlators from shape deformations in Cubic Curvature Gravity

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arxiv 2208.00093 v2 pith:AYKZINBO submitted 2022-07-29 hep-th gr-qc

CFT correlators from shape deformations in Cubic Curvature Gravity

classification hep-th gr-qc
keywords entropyobtainedcurvatureentanglementgravitycftscoefficientscorrelators
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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We find a covariant expression for the universal part of the holographic entanglement entropy which is valid for CFTs dual to generic higher curvature gravities in up to five bulk dimensions. We use this functional to compute universal coefficients of stress-tensor correlators in three-dimensional CFTs dual to Cubic Curvature Gravity. Using gauge/gravity duality, we work out an expression for the entanglement entropy of deformed entangling regions and read the coefficients from the power expansion of the entropy in the deformation parameter. In particular, we obtain the $t_4$ coefficient of the 3-point function and exhibit a difference between the results obtained using the entanglement entropy functional for minimal and non-minimal splittings. We compare the obtained expressions for $t_{4}$ derived considering both splittings with results obtained through other holographic methods which are splitting-independent. We find agreement with the result obtained from the non-minimal splitting, whereas the result derived from the minimal splitting is inconsistent and it is therefore ruled out.

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Cited by 2 Pith papers

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  1. Universality of pseudoentropy for deformed spheres in dS/CFT

    hep-th 2025-12 conditional novelty 6.0

    The quadratic shape-deformation correction to pseudoentropy in dS/CFT is controlled by the analytically continued stress-tensor coefficient C_T, making the sphere a local extremum across Einstein and quadratic-curvatu...

  2. Renormalized pseudoentropy in dS/CFT

    hep-th 2026-02 conditional novelty 5.0

    Renormalized holographic pseudoentropy in dS/CFT is constructed from conformal-gravity actions in four and six dimensions, yielding finite sphere values and Mezei-like shape dependence for small deformations.