The spinless modular bootstrap at large central charge
Version 1 / Nov 07, 2026 / CC BY 4.0
Abstract
The spinless modular bootstrap bounds the dimension of the lightest primary other than the vacuum in a two-dimensional conformal field theory, using only modular invariance of the torus partition function at zero angular potential. For unitary, compact theories with central charge and no conserved currents beyond the Virasoro algebra, these bounds read at large . The best slope was known only to lie between and , where the bound would reach the BTZ black hole threshold. We show that it is exactly . No linear functional in a class that contains all finite combinations of derivatives improves on by more than , and an explicit functional gives for all sufficiently large . The value has an electrostatic origin: as a function of a complexified dimension, of a functional is a two-dimensional potential with positive charges at the zeros of . Positivity forces to fall as fast as the Cardy density of states grows, and the maximum principle bounds the potential by an explicit harmonic function, which fixes . The field of this potential is the spectral curve of a mean-field theory of the optimal functionals, and its charge density is the distribution that the zeros of any functionals attaining must follow. We also conjecture the coefficient of the correction to the optimal bound, supported by numerics up to .
Provenance statement
References
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