Geometry of Conformal Manifolds and the Inversion Formula
arXiv:2212.11186 · doi:10.1007/JHEP07(2023)205
Abstract
Families of conformal field theories are naturally endowed with a Riemannian geometry which is locally encoded by correlation functions of exactly marginal operators. We show that the curvature of such conformal manifolds can be computed using Euclidean and Lorentzian inversion formulae, which combine the operator content of the conformal field theory into an analytic function. Analogously, operators of fixed dimension define bundles over the conformal manifold whose curvatures can also be computed using inversion formulae. These results relate curvatures to integrated four-point correlation functions which are sensitive only to the behavior of the theory at separated points. We apply these inversion formulae to derive convergent sum rules expressing the curvature in terms of the spectrum of local operators and their three-point function coefficients. We further show that the curvature can smoothly diverge only if a conserved current appears in the spectrum, or if the theory develops a continuum. We verify our results explicitly in examples. In particular, for (2,2) superconformal field theories we derive a lower bound on the scalar curvature, which is saturated by free theories when the central charge is a multiple of three.
48 pages
References in corpus (7)
- Sphere Partition Functions and the Zamolodchikov Metric
- equations, localization and exact chiral rings in 4d N=2 SCFTs
- New Modular Invariants in Super-Yang-Mills Theory
- Tackling the SDC in AdS with CFTs
- The chiral ring of AdS3/CFT2 and the attractor mechanism
- Harnessing S-Duality in SYM & Supergravity as -Averaged Strings
- On non-supersymmetric conformal manifolds: field theory and holography