The thermal bootstrap for the critical O(N) model
arXiv:2411.00978 · doi:10.1103/PhysRevLett.134.211604
Abstract
We propose a numerical method to estimate one-point functions and the free-energy density of conformal field theories at finite temperature by solving the Kubo-Martin-Schwinger condition for the two-point functions of identical scalars. We apply the method for the critical O(N) model for N = 1,2,3 in 3 d 4. We find agreement with known results from Monte Carlo simulations and previous results for the 3d Ising model, and we provide new predictions for N = 2,3.
5 pages plus supplemental material, refs. updated
References in corpus (22)
- N=6 superconformal Chern-Simons-matter theories, M2-branes and their gravity duals
- The Lightcone Bootstrap and the Spectrum of the 3d Ising CFT
- Universal scaling functions of critical Casimir forces obtained by Monte Carlo simulations
- Bootstrapping Heisenberg Magnets and their Cubic Instability
- Critical exponents of the 3d Ising and related models from Conformal Bootstrap
- Conformal field theories at non-zero temperature: operator product expansions, Monte Carlo, and holography
- The critical O(N) CFT: Methods and conformal data
- Strange metals and the AdS/CFT correspondence
- Integrability and Conformal Bootstrap: One Dimensional Defect CFT
- Truncatable bootstrap equations in algebraic form and critical surface exponents
- The Lorentzian inversion formula and the spectrum of the 3d O(2) CFT
- Rigorous bounds on irrelevant operators in the 3d Ising model CFT
- Large Partition Functions of the ABJM Theory
- Universal Asymptotics for High Energy CFT Data
- Bootstrapping the 3d Ising Stress Tensor
- New Developments in the Numerical Conformal Bootstrap
- Black hole bulk-cone singularities
- Thermal one-point functions and single-valued polylogarithms
- Improving the five-point bootstrap
- Conformal graphs as twisted partition functions
- Easy bootstrap for the 3D Ising model: a hybrid approach of the lightcone bootstrap and error minimization methods
- Conformal line defects at finite temperature