Skip to content
DraconiticResearch
Search Sources API
182,544 studies31 sourcesUpdated 3 min ago
PreprintCC BY 4.0arXiv

Stochastic Gradient Leimkuhler-Matthews Integrator with Second Order Discretization Error

Abstract

Stochastic gradient Langevin dynamics (SGLD) has a discretization error of first order in the step size h, even with the full gradient. We study the stochastic gradient Leimkuhler-Matthews (SGLM) integrator, which has the same cost as SGLD, one stochastic gradient per step, and reuses each Gaussian vector in consecutive steps. With the full gradient, SGLM is the Leimkuhler-Matthews (LM) integrator, whose discretization error for the invariant distribution is of second order. For a potential strongly convex outside a ball, we prove the bound 𝒪(1/Nh + Σ2 h2 + h4) on the mean square error (MSE) of time averages of SGLM over N steps, where Σ bounds the variance of the gradient noise. The proof uses a modified class that absorbs the non-Markovian part of SGLM. The discretization error enters this bound as h4 and the MSE bound of SGLD as h2, while a larger batch reduces only the term Σ2 h2 in both bounds. In Bayesian logistic regression on MNIST, SGLM has a smaller estimated MSE than SGLD. The coefficient of h in the numerical bias of SGLM is given explicitly by the covariance of the gradient noise and the continuous Poisson equation. The coefficient for SGLD contains in addition the Hessian of the potential, which comes from the discretization error. Through Riesz representors, the coefficients of the numerical bias determine the coefficients of the Wasserstein-1 errors of SGLM and SGLD.

Related

  1. Strong error analysis of a stochastic exponential integrator for SPDEs driven by fractional Brownian motion with H<1/2
    Antoine Tambue, Aurelien Junior Noupelah, Louis Aime Fono
    arXivPreprintarXiv licenceFull textNumerical analysis & scientific computingProbabilityarXiv
  2. Finite volume discretization and normalized gradient flow for computing minimizers of the rotating Gross-Pitaevskii energy
    Quentin Chauleur, Guillaume Dujardin, Robin Roussel
    HALPreprintCC BY 4.0Full textNumerical analysis & scientific computingHALarXiv
  3. Numerical Methods for Dynamical Low-Rank Approximations of Stochastic Differential Equations -- Part II: Stochastic discretization
    Yoshihito Kazashi, Fabio Nobile, Fabio Zoccolan
    arXivPreprintarXiv licenceFull textNumerical analysis & scientific computingarXiv
  4. Random attractors and almost-sure stability under discretization of a stochastic autoparametric system
    Chuchu Chen, Jialin Hong, Yibo Wang
    arXivPreprintarXiv licenceFull textDynamical systemsNumerical analysis & scientific computingarXiv
  5. Latent Ornstein–Uhlenbeck-Driven Log-ARCH Models: Continuous-Time Stochastic Dynamics, Exact Discretization, and Long-Span QML Theory
    Yue Su
    MathematicsPeer-reviewedCC BY 4.0General mathematicsCrossref
BibTeX
@misc{ye2026stochastic,
  title = {{Stochastic Gradient Leimkuhler-Matthews Integrator with Second Order Discretization Error}},
  author = {Xuda Ye and Yuliang Wang and Guang Lin and Cindy Xiangrui Kong},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.24781},
  eprint = {2610.24781},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.24781},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Stochastic Gradient Leimkuhler-Matthews Integrator with Second Order Discretization Error
AU  - Xuda Ye
AU  - Yuliang Wang
AU  - Guang Lin
AU  - Cindy Xiangrui Kong
PY  - 2026
DA  - 2026/10/17
PB  - arXiv
DO  - 10.48550/arxiv.2610.24781
UR  - https://arxiv.org/abs/2610.24781
AB  - Stochastic gradient Langevin dynamics (SGLD) has a discretization error of first order in the step size h, even with the full gradient. We study the stochastic gradient Leimkuhler-Matthews (SGLM) integrator, which has the same cost as SGLD, one stochastic gradient per step, and reuses each Gaussian vector in consecutive steps. With the full gradient, SGLM is the Leimkuhler-Matthews (LM) integrator, whose discretization error for the invariant distribution is of second order. For a potential strongly convex outside a ball, we prove the bound 𝒪(1/Nh + Σ^2 h^2 + h^4) on the mean square error (MSE) of time averages of SGLM over N steps, where Σ bounds the variance of the gradient noise. The proof uses a modified class that absorbs the non-Markovian part of SGLM. The discretization error enters this bound as h^4 and the MSE bound of SGLD as h^2, while a larger batch reduces only the term Σ^2 h^2 in both bounds. In Bayesian logistic regression on MNIST, SGLM has a smaller estimated MSE than SGLD. The coefficient of h in the numerical bias of SGLM is given explicitly by the covariance of the gradient noise and the continuous Poisson equation. The coefficient for SGLD contains in addition the Hessian of the potential, which comes from the discretization error. Through Riesz representors, the coefficients of the numerical bias determine the coefficients of the Wasserstein-1 errors of SGLM and SGLD.
ER  -