A spectral gap throughout the high-temperature Sherrington–Kirkpatrick phaseResearch Paper
Motivation
The Sherrington–Kirkpatrick (SK) model (1975) is the basic mean-field spin glass: Ising spins interact through independent Gaussian couplings of variance , so each spin is weakly coupled to every other one with random signs. The model is the testing ground for questions about disordered systems, about sampling from Gibbs measures, and about the performance of Markov chain Monte Carlo. A central question is whether Glauber (heat-bath) dynamics, which resamples one spin at a time from its conditional law, relaxes at a rate independent of the system size. Equivalently: does the Gibbs measure satisfy a dimension-free Poincaré inequality with respect to the heat-bath Dirichlet form?
The equilibrium high-temperature phase is , where the free energy equals its annealed value (Aizenman, Lebowitz and Ruelle 1987). Dynamical results had reached only part of this range.
Timeline
- 1963. Glauber introduces local stochastic spin dynamics (doi:10.1063/1.1703954).
- 1975. Sherrington and Kirkpatrick introduce the model (doi:10.1103/PhysRevLett.35.1792).
- 1987. Aizenman, Lebowitz and Ruelle prove the annealed free energy for all (doi:10.1007/BF01217677).
- 2006. Wu proves Poincaré inequalities under a Dobrushin-type condition (doi:10.1214/009117906000000368).
- 2019. Bauerschmidt and Bodineau prove a high-temperature log-Sobolev inequality for a different (full spin-flip) Dirichlet form (doi:10.1016/j.jfa.2019.01.007).
- 2022. Eldan, Koehler and Zeitouni give a spectral condition yielding a heat-bath gap for (doi:10.1007/s00440-021-01085-x); Anari, Jain, Koehler, Pham and Vuong prove mixing in the same range (arXiv:2106.04105).
- 2024. Anari, Koehler and Vuong extend this to (doi:10.1145/3618260.3649622); Adhikari, Brennecke, Xu and Yau obtain gaps for mixed -spin models under a small-coefficient condition (doi:10.1007/s00440-024-01261-9); El Alaoui and Gaitonde, and Brennecke, Schertzer, Xu and Yau, control the spin covariance for all (arXiv:2212.02445, doi:10.2140/pmp.2024.5.131).
- 2026. Wang proves optimal mixing for (arXiv:2608.22159); Boban, Li and Oveis Gharan reach (arXiv:2609.13138).
The source of this mission is an OpenAI preprint dated September 24, 2026, which treats every fixed .
Setting
Fix . Let be a symmetric matrix with zero diagonal and independent entries for . The zero-field Gibbs law on is
Let be the conditional expectation under given all spins except ; it averages over and its -th flip with Gibbs weights. The unscaled Dirichlet form is
The discrete heat-bath chain picks a uniform site and resamples it, with transition operator ; its spectral gap is over nonconstant .
Formalization targets
Goal: Theorem 1.1
There is a finite constant such that
and consequently the discrete heat-bath chain has spectral gap at least with probability tending to one. Lean: OAI.SKGap.sk_main, open on the platform.
Significance
The theorem gives a size-independent relaxation time for continuous-time heat-bath dynamics (rate-one clocks) throughout the high-temperature phase, for every observable simultaneously on one disorder event. It extends the dynamical picture from to the full equilibrium range , where only linear-observable (covariance) control was previously known. A Poincaré inequality is the input for mixing bounds and for companion results on cutoff and critical slowing down.
The result is proved in an OpenAI preprint; it has not been peer reviewed, and no machine-checked proof exists.
Difficulty
Dobrushin-type influence bounds fail because the sum of absolute couplings at a site grows like ; any argument must exploit cancellations from the random signs. Covariance bounds control only linear observables, while the Poincaré inequality must hold for all -dimensional families of test functions at once. The natural route through stochastic localization runs into rare observation events: an event of exponentially small probability can still carry most of the variance of a particular test function, and invertibility of the field equation must hold at every sufficiently accurate solution along the observation path.
Formalization scope
- Spins are
Fin n → Bool, withspinValuemapping to ; couplings are indexed by pairs (Edge n) and symmetrized with zero diagonal bycoupling. hamiltonian g 0 x = ½ ∑_{i,k} x_i J_{ik} x_k;mass,expectation,varianceare exact finite sums over .conditionalExpectation g h i f xis the two-point Gibbs average over and its -th flip;dirichletis the unscaled form .disorderLaw β n = Measure.pi (fun _ => gaussianReal 0 (β^2/n))over the edges (variance ).discreteGap gis the infimum of over with positive variance.MainStatement βasserts a single for which both the Poincaré event and the gap event have probability tending to .
Formalization needs Gaussian product measures, finite Gibbs measures and heat-bath operators, and the analysis behind the proof: matrix concentration, TAP/AMP-type field recursions and stochastic localization. Formal versions of the paper's intermediate results (for example Proposition 8.3, the terminal observation gap) are welcome.
Selected references
- OpenAI, A spectral gap throughout the high-temperature Sherrington–Kirkpatrick phase, preprint, September 24, 2026. https://github.com/openai/math/blob/adc7f1241b42e322a6451854ab7e4b4c146bf78a/preprints/A-spectral-gap-throughout-the-high-temperature-Sherrington-Kirkpatrick-phase-September-24-2026/main.pdf
- D. Sherrington, S. Kirkpatrick, Solvable model of a spin-glass, Phys. Rev. Lett., 1975. https://doi.org/10.1103/PhysRevLett.35.1792
- M. Aizenman, J. L. Lebowitz, D. Ruelle, Some rigorous results on the Sherrington–Kirkpatrick spin glass model, Comm. Math. Phys., 1987. https://doi.org/10.1007/BF01217677
- R. Eldan, F. Koehler, O. Zeitouni, A spectral condition for spectral gap: fast mixing in high-temperature Ising models, Probab. Theory Related Fields, 2022. https://doi.org/10.1007/s00440-021-01085-x
- N. Anari, F. Koehler, T.-D. Vuong, Trickle-down in localization schemes and applications, STOC 2024. https://doi.org/10.1145/3618260.3649622
- S. Wang, Optimal mixing of Glauber dynamics for the Sherrington–Kirkpatrick model at , preprint, 2026. https://arxiv.org/abs/2608.22159
- M. Boban, A. Li, S. Oveis Gharan, Rank-1-perturbed trickledown theorems, preprint, 2026. https://arxiv.org/abs/2609.13138
- C. Brennecke, A. Schertzer, C. Xu, H.-T. Yau, The two point function of the SK model without external field at high temperature, Probab. Math. Phys., 2024. https://doi.org/10.2140/pmp.2024.5.131
- Y. Chen, R. Eldan, Localization schemes: a framework for proving mixing bounds for Markov chains, Duke Math. J., 2025. https://doi.org/10.1215/00127094-2024-0063
- R. Eldan, Thin shell implies spectral gap up to polylog via a stochastic localization scheme, Geom. Funct. Anal., 2013. https://doi.org/10.1007/s00039-013-0214-y