Ergodicity and error estimate of laws for a random splitting Langevin Monte Carlo
Lei Li, Chen Wang, Mengchao Wang
TL;DR
This work introduces the randomized splitting Langevin Monte Carlo (RSLMC), a simple random-order Lie–Trotter splitting of Langevin dynamics designed to reduce the first-order bias of standard Langevin Monte Carlo. The authors develop a rigorous framework based on relative entropy and semigroup commutators to quantify finite-time discretization errors, and establish a uniform-in-time bound by proving geometric ergodicity through reflection coupling, yielding $W_1$-convergence of order $O(\tau^2)$. They further obtain sharp finite-time relative-entropy bounds of order $O(\tau^4)$ and derive polynomial-in-$|x|$ bounds for the gradient and Hessian of the log-density, ensuring robust density control and applicability to nonconvex settings. Numerical experiments in 1D and 2D validate the theory, demonstrating fourth-order convergence in KL divergence and confirming the method’s practical efficacy with modest extra cost compared to standard LMC.
Abstract
The random splitting Langevin Monte Carlo could mitigate the first order bias in Langevin Monte Carlo with little extra work compared other high order schemes. We develop in this work an analysis framework for the sampling error under Wasserstein distance regarding the random splitting Langevin Monte Carlo. First, the sharp local truncation error is obtained by the relative entropy approach together with the explicit formulas for the commutator of related semi-groups. The necessary pointwise estimates of the gradient and Hessian of the logarithmic density are established by the Bernstein type approach in PDE theory. Second, the geometric ergodicity is established by accommodation of the reflection coupling. Combining the ergodicity with the local error estimate, we establish a uniform-in-time sampling error bound, showing that the invariant measure of the method approximates the true Gibbs distribution with $O(τ^2)$ accuracy where $τ$ is the time step. Lastly, we perform numerical experiments to validate the theoretical results.
