Abstract

This review treats the mathematical and algorithmic foundations of non-reversible Markov chains in the context of event-chain Monte Carlo (ECMC), a continuous-time lifted Markov chain that employs the factorized Metropolis algorithm. It analyzes a number of model applications and then reviews the formulation as well as the performance of ECMC in key models in statistical physics. Finally, the review reports on an ongoing initiative to apply ECMC to the sampling problem in molecular simulation, i.e., to real-world models of peptides, proteins, and polymers in aqueous solution.

Highlights

  • Markov-chain Monte Carlo (MCMC) is an essential tool for the natural sciences

  • The distribution π {t} depends on the initial distribution, but for any choice of π {0}, for an irreducible and aperiodic transition matrix, the total variation distance is smaller than an exponential bound Cαt with α ∈ (0, 1)

  • The conductance yields the considerable diffusive-to-ballistic speedup that may be reached by a non-reversible lifting if the collapsed Markov chain is itself close to the ∼ 1/ 2 upper bound of Equations (11) and (13)

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Summary

INTRODUCTION

Markov-chain Monte Carlo (MCMC) is an essential tool for the natural sciences. It is the subject of a research discipline in mathematics. The Metropolis or the heatbath (Gibbs-sampling) algorithms are popular choices They generally compute acceptance probabilities from the changes in the total potential (the system’s energy) and mimic the behavior of physical systems in the thermodynamic equilibrium. Event-chain Monte Carlo (ECMC) [7, 8] is a family of local, non-reversible MCMC algorithms developed over the last decade. This remains within the framework of (memoryless) Markov chains.

Transition Matrices and Balance
Irreducibility and Convergence—Basic
Factorization
Stochastic Potential Switching
Lifting
Particle Lifting
N in the collapsed
Thinning
Thinning and Bounding Potentials
SINGLE PARTICLES ON A PATH GRAPH
Bounded One-Dimensional
Square-Wave Stationary Distribution
Unbounded One-Dimensional
N PARTICLES IN ONE DIMENSION
Reversible MCMC in One-Dimensional
Continuous One-Dimensional Reversible
Non-reversible MCMC in
Discrete Non-reversible MCMC in One
Continuous Non-reversible MCMC in One
Event-Chain Monte Carlo in
Factor-Field ECMC in One Dimension
STATISTICAL-MECHANICS MODELS IN
Two-Dimensional Hard Disks
Parallel Hard-Disk ECMC
Harmonic Model
Physics of the Harmonic Model
ECMC Algorithm for the Harmonic Model
Event-Chain Monte Carlo for Continuous Spin Models
Spin Waves and Topological Excitations in the
Relaxation Time Scales in Spin Models
ECMC AND MOLECULAR SIMULATION
Theoretical Aspects of ECMC for
JeLLyFysh Application for ECMC
PROSPECTS
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