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Scalable Generative Sampling and Multilevel Estimation for Lattice Field Theories Near Criticality

Published 11 Apr 2026 in hep-lat, cond-mat.stat-mech, and physics.comp-ph | (2604.10209v1)

Abstract: Sampling lattice field theories near criticality is severely hindered by critical slowing down, which makes standard Markov chain methods increasingly inefficient at large lattice volumes. We introduce a multiscale generative sampler, inspired by renormalization-group ideas, that models the Boltzmann distribution through a coarse-to-fine hierarchy across length scales. At each level, a conditional Gaussian mixture model captures the main local dependence of newly introduced variables on the already-sampled coarse field, while a masked continuous normalizing flow refines the remaining conditional structure. Coarse levels encode the dominant long-wavelength modes, and finer levels progressively add short-distance fluctuations. In addition, because the architecture preserves coarse fields exactly during refinement, it provides exact restriction maps at no additional computational cost and directly enables unbiased Multilevel Monte Carlo (MLMC) variance reduction. For the two-dimensional scalar $φ4$ theory at criticality, the method achieves integrated autocorrelation times orders of magnitude smaller than Hybrid Monte Carlo (HMC) on large volumes, maintains high importance-sampling efficiency relative to other generative baselines, and reproduces unbiased physical observables in statistical agreement with long HMC simulations.

Summary

  • The paper introduces a multiscale generative framework that decomposes the Boltzmann measure, reducing critical slowing down.
  • It employs conditional Gaussian mixtures and normalizing flows, achieving nearly constant autocorrelation times even at large lattice sizes.
  • The approach integrates MLMC variance reduction via exact coarse-to-fine restrictions, outperforming HMC in efficiency and precision.

Scalable Multiscale Generative Sampling for Critical Lattice Field Theories

Introduction and Motivation

Sampling lattice field configurations near criticality is a central problem in computational physics, underlying the first-principles estimation of physical observables in quantum field theories and statistical mechanics. Traditional Markov Chain Monte Carlo (MCMC) methods such as Hybrid Monte Carlo (HMC) exhibit severe inefficiency in the critical regime. The autocorrelation time increases polynomially with the correlation length ξ\xi (with dynamical exponent z2z\sim2 for HMC in scalar theory), yielding sharply increased computational cost as system size and criticality are approached.

Recent progress in machine learning–driven generative modeling, especially via normalizing flows (NFs), has provided alternatives that bypass Markov chain correlations and enable efficient parallelized proposals. However, these models struggle to scale at criticality—their representational and computational demands scale poorly with increasing system size, particularly for single-scale architectures that must capture all correlations at once. This work introduces a multiscale generative framework explicitly designed to decompose and model the hierarchical structure of critical lattice systems, achieving improved scalability, efficiency, and statistical accuracy.

Multilevel Coarse-to-Fine Generative Modeling

Theoretical Framework

The method is inspired by renormalization-group (RG) concepts: long-wavelength (infrared) modes are encoded at successively coarser representations, while short-wavelength fluctuations are introduced via finer-scale refinements. The proposed generative decomposition expresses the Boltzmann measure as a product of conditional distributions across levels, forming a coarse-to-fine sampling hierarchy. At each upsampling step, the newly introduced degrees of freedom are generated conditionally on the previously sampled (coarser) field:

q(ϕ)=q0(ϕ(0))=1maxq(ϕ()ϕ(1))q(\phi) = q_0(\phi^{(0)}) \prod_{\ell=1}^{\ell_{\text{max}}} q_\ell \left( \phi^{(\ell)} \mid \phi^{(\leq \ell-1)} \right)

where ϕ(0)\phi^{(0)} is the coarsest lattice, and each qq_\ell models the conditional distribution for new sites at scale \ell given all previously sampled sites. This factorization enables strictly local or short-range conditional dependencies at each scale, bypassing the need for large receptive fields in the generative network even at large system sizes. Figure 1

Figure 1: Kadanoff-inspired multilevel partition of a periodic lattice into coarse, intermediate, and fine sites, visually delineating the generative coarse-to-fine decomposition.

Generative Components

  • Conditional Gaussian Mixture Models (GMMs): For each refinement, a local conditional GMM rapidly approximates the leading structure of the distribution for new variables given their coarse neighbors; this factorizes for efficiency and tractability.
  • Conditional Normalizing Flows (CNFs): To overcome limitations of GMM expressivity, the samples are further refined by conditional CNFs parameterized by neural ODEs, enhancing their fit to the true conditional Boltzmann weights while preserving analytic tractability for importance sampling.

This hierarchical design ensures that coarse fields are preserved exactly during each refinement step, enabling an exact restriction from fine to coarse representations at no extra cost—a crucial property for downstream variance reduction via multilevel control variates.

Numerical Results: 2D ϕ4\phi^4 Theory at Criticality

The methodology is evaluated on two-dimensional scalar ϕ4\phi^4 theory at its critical coupling. The critical slowing down of HMC is severe in this regime, with autocorrelation time scaling as L1.99\sim L^{1.99} in system size. The study benchmarks the proposed scheme against baselines including HMC, dense-CNF, Hutch CNF, and the Super Resolving (SR-NF) hierarchical flow.

Numerical highlights:

  • The integrated autocorrelation time for magnetization, τint(m)\tau_{\rm int}(|m|), remains nearly flat (z2z\sim20) up to z2z\sim21 for the new multiscale method, while HMC rises to z2z\sim22 and SR-NF surges at large z2z\sim23.
  • At z2z\sim24, the method still beats HMC by a factor of z2z\sim25 in autocorrelation time and z2z\sim26 in wall-clock time to reach HMC statistical precision for physical observables.
  • The effective sample size per generated configuration remains robust for the new model, even as rivals like SR-NF collapse at high z2z\sim27 due to shallow or non-hierarchical generative policies.

Statistical Consistency

A critical test is whether the generative model, combined with importance weights, yields unbiased results for physical observables relative to HMC. The method's self-normalized IS estimates for the connected susceptibility z2z\sim28 are in agreement with direct HMC values within z2z\sim29–q(ϕ)=q0(ϕ(0))=1maxq(ϕ()ϕ(1))q(\phi) = q_0(\phi^{(0)}) \prod_{\ell=1}^{\ell_{\text{max}}} q_\ell \left( \phi^{(\ell)} \mid \phi^{(\leq \ell-1)} \right)0 across all q(ϕ)=q0(ϕ(0))=1maxq(ϕ()ϕ(1))q(\phi) = q_0(\phi^{(0)}) \prod_{\ell=1}^{\ell_{\text{max}}} q_\ell \left( \phi^{(\ell)} \mid \phi^{(\leq \ell-1)} \right)1, while baseline methods deteriorate at large lattice size. Figure 2

Figure 2: Relative deviation of the connected susceptibility from HMC, q(ϕ)=q0(ϕ(0))=1maxq(ϕ()ϕ(1))q(\phi) = q_0(\phi^{(0)}) \prod_{\ell=1}^{\ell_{\text{max}}} q_\ell \left( \phi^{(\ell)} \mid \phi^{(\leq \ell-1)} \right)2, as a function of system size q(ϕ)=q0(ϕ(0))=1maxq(ϕ()ϕ(1))q(\phi) = q_0(\phi^{(0)}) \prod_{\ell=1}^{\ell_{\text{max}}} q_\ell \left( \phi^{(\ell)} \mid \phi^{(\leq \ell-1)} \right)3 for various models.

Multilevel Monte Carlo (MLMC) Variance Reduction

A further advantage of the hierarchical approach is its compatibility with the MLMC estimator framework. The exact restriction property means that multiple levels of the hierarchy can serve as correlated control variates, systematically reducing estimator variance at fixed computational budget. The variance reduction observed for observables such as magnetization corresponds, for example, to a q(ϕ)=q0(ϕ(0))=1maxq(ϕ()ϕ(1))q(\phi) = q_0(\phi^{(0)}) \prod_{\ell=1}^{\ell_{\text{max}}} q_\ell \left( \phi^{(\ell)} \mid \phi^{(\leq \ell-1)} \right)4 wall-time saving at q(ϕ)=q0(ϕ(0))=1maxq(ϕ()ϕ(1))q(\phi) = q_0(\phi^{(0)}) \prod_{\ell=1}^{\ell_{\text{max}}} q_\ell \left( \phi^{(\ell)} \mid \phi^{(\leq \ell-1)} \right)5 compared to plain importance sampling.

Implications, Limitations, and Future Directions

This work demonstrates that explicit multiscale decompositions, rooted in RG structure and implemented with hybrid probabilistic deep learning, provide a robust pathway for scalable, statistically sound generative modeling of critical lattice distributions. The significant reduction in autocorrelation and computational expense at large scales represents a tangible step forward for both statistical physics and quantum field theory computations.

Key implications:

  • Computational efficiency: Applicable to system sizes and regimes where baseline generative models and HMC are ineffective, enabling precision studies of larger and more complex field theories.
  • Generalizability: The modular design—separating coarse modeling, fine-graining, and flow-based refinement—suggests adaptability for gauge theories, higher dimensions, or even quantum many-body applications.
  • Control variate integration: The exact restriction property is unmatched by full-lattice CNF upsampling (noisier or incurably expensive backtracking), further incentivizing the use of masked, locality-preserving designs in probabilistic modeling for critical phenomena.

Limitations and prospects:

  • The decrease in importance-sampling efficiency at very large q(ϕ)=q0(ϕ(0))=1maxq(ϕ()ϕ(1))q(\phi) = q_0(\phi^{(0)}) \prod_{\ell=1}^{\ell_{\text{max}}} q_\ell \left( \phi^{(\ell)} \mid \phi^{(\leq \ell-1)} \right)6 signals the need for larger or better-trained fine-level models.
  • Future work should address capacious modeling for group-valued variables (e.g., gauge field configurations), and further exploit the synergy between machine learning and classical multiscale statistical mechanics.

Conclusion

The multilevel generative sampling framework presented in "Scalable Generative Sampling and Multilevel Estimation for Lattice Field Theories Near Criticality" (2604.10209) resolves key bottlenecks for lattice simulation near criticality. By aligning generative modeling with renormalization principles and exploiting hierarchical conditional dependencies, the approach achieves orders-of-magnitude improvement in sampling efficiency and estimator precision. Its design principles are broadly relevant for domains requiring scalable, unbiased inference from high-dimensional, correlated distributions, and are poised for further impact as generative modeling techniques merge with multiscale physical theory.

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