Torus one-point functions of primary fields in critical loop models are infinite sums of conformal blocks whose coefficients are products of double Gamma functions and polynomials in the loop weight, obtained via numerical bootstrap from sphere four-point functions at different central charge.
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Conjecture of an exact formula for 3-point functions of ℓ-leg and diagonal fields in critical loop models, supported by transfer-matrix numerics on cylinders that agree in most cases.
GenMed uses diffusion models to capture P(X,Y) for medical tasks and performs inference via gradient-based test-time optimization, supporting arbitrary observation combinations without retraining.
Analytic continuation of known conformal data from the Q≤4 Potts loop model yields complex CFTs describing the model for Q>4 and complex Q with suitable complex couplings, supported by transfer-matrix checks.
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Torus one-point functions in critical loop models
Torus one-point functions of primary fields in critical loop models are infinite sums of conformal blocks whose coefficients are products of double Gamma functions and polynomials in the loop weight, obtained via numerical bootstrap from sphere four-point functions at different central charge.
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Three-point functions in critical loop models
Conjecture of an exact formula for 3-point functions of ℓ-leg and diagonal fields in critical loop models, supported by transfer-matrix numerics on cylinders that agree in most cases.
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GenMed: A Pairwise Generative Reformulation of Medical Diagnostic Tasks
GenMed uses diffusion models to capture P(X,Y) for medical tasks and performs inference via gradient-based test-time optimization, supporting arbitrary observation combinations without retraining.
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Making complex CFTs real: The two-dimensional Potts model for $Q>4$ and complex $Q$
Analytic continuation of known conformal data from the Q≤4 Potts loop model yields complex CFTs describing the model for Q>4 and complex Q with suitable complex couplings, supported by transfer-matrix checks.