Journal Article10.1016/0370-2693(87)91197-X
Hybrid Monte Carlo
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TL;DR: In this article, a hybrid (molecular dynamics/Langevin) algorithm is used to guide a Monte Carlo simulation of lattice field theory, which is especially efficient for quantum chromodynamics which contain fermionic degrees of freedom.
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About: This article is published in Physics Letters B. The article was published on 03 Sep 1987. The article focuses on the topics: Hybrid Monte Carlo & Quantum Monte Carlo.
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References
Equation of state calculations by fast computing machines
TL;DR: In this article, a modified Monte Carlo integration over configuration space is used to investigate the properties of a two-dimensional rigid-sphere system with a set of interacting individual molecules, and the results are compared to free volume equations of state and a four-term virial coefficient expansion.
Stochastic quantization versus the microcanonical ensemble: Getting the best of both worlds
TL;DR: It is argued that the new proposal always represents a significant improvement over a Langevin simulation, and may even improve over the microcanonical method, in which case only a trivial code modification is required.
Acceleration of gauge field dynamics
TL;DR: In this paper, it was shown that the success of acceleration for abelian gauge field dynamics need not depend on any choice of gauge and proposed a particular scheme for acceleration in non-abelian theories which is also gauge independent.
Hybrid Molecular Dynamics Algorithms for the Numerical Simulation of Quantum Chromodynamics
TL;DR: Two algorithms for the numerical simulation of SU(3) lattice gauge theory with dynamical quarks are discussed, based on the hybrid stochastic method of Duane and Kogut, which allow the simulation of arbitrary numbers of quarks.
Langevin simulations of lattice field theories
G. George Batrouni,G. R. Katz,Andreas S. Kronfeld,G. P. Lepage,B. Svetitsky,Kenneth G. Wilson +5 more
TL;DR: Fourier techniques that greatly accelerate simulations on large lattices and a new technique for including quark vacuum-polarization corrections that admits any number of flavors, odd or even, without the need for nested Monte Carlo calculations are introduced.