Use the exact Kac–Ward conditional sampler as an oracle teacher for a neural autoregressive distribution over planar Ising configurations. At each prefix, supervise the network with the exact next-spin probability rather than only a sampled next spin, then retain the oracle as an evaluation and active-correction mechanism for prefixes where the student is inaccurate. This converts an approximate variational sampler into a calibrated amortized approximation with an exact, independently sampled…
Add calibrated multiplicative noise to a binary energy-based model, Hopfield network, or discrete recurrent attractor system so that its effective coupling follows a chosen distance from the collective critical point. Unlike ordinary temperature annealing, the controller distinguishes microscopic channel noise from Gibbs or sampling noise and predicts when ordered attractors should disappear through a measurable susceptibility peak.
Attach an exact structural uncertainty report to any best-of-N evaluation: after measuring reliability only for budgets n = 1,...,m, report that deployment reliability at budget N is unresolved by at least B_{m,N}. Use this width to select the smallest audit budget that makes a claimed reliability gap meaningful, or reject model comparisons whose validation budget lies below the square-root-of-N threshold.
Equip an autoregressive model with a hard constraint that generated token ranks cannot contain a nondecreasing subsequence of length k. Maintain a patience-sorting-style state representing the smallest ending token rank achievable by subsequences of lengths 1 through k-1, mask tokens that would create a length-k subsequence, and optionally sample uniformly among valid continuations using exact suffix counts. This provides a mathematically controlled data-augmentation or decoding regime for…
Represent a set of neural prototypes, mixture components, or latent particles by N points in R^2, and initialize or refresh them with Langevin dynamics targeting a quadratically confined logarithmic Coulomb gas. The logarithmic repulsion prevents particle collapse, while the paper's N-uniform logarithmic Sobolev inequality predicts that mixing need not degrade as the particle bank grows.
Replace a fixed discrete augmentation distribution over a finite symmetry group by a continuous-time random walk driven by learnable symmetric Poisson jump rates. Use the resulting transformed-example distribution as a symmetry regularizer, with an even ℓ^{2m} distance to uniformity whose behavior is guaranteed to improve monotonically as the symmetric rates increase for the group families covered by the paper.
Put a gradient-Gibbs prior on differences between connected neural parameters rather than on individual parameters, and evolve the parameters with Langevin steps generated from randomly selected strictly convex component energies. The aggregate regularizer may be non-convex, but every sampled component has controlled curvature and outward drift, providing a practical stability mechanism for noisy training.