TY - JOUR
T1 - Langevin dynamics neglecting detailed balance condition
AU - Ohzeki, Masayuki
AU - Ichiki, Akihisa
N1 - Publisher Copyright:
© 2015 American Physical Society.
PY - 2015/7/6
Y1 - 2015/7/6
N2 - An improved method for driving a system into a desired distribution, for example, the Gibbs-Boltzmann distribution, is proposed, which makes use of an artificial relaxation process. The standard techniques for achieving the Gibbs-Boltzmann distribution involve numerical simulations under the detailed balance condition. In contrast, in the present study we formulate the Langevin dynamics, for which the corresponding Fokker-Planck operator includes an asymmetric component violating the detailed balance condition. This leads to shifts in the eigenvalues and results in the acceleration of the relaxation toward the steady state. The numerical implementation demonstrates faster convergence and shorter correlation time, and the technique of biased event sampling, Nemoto-Sasa theory, further highlights the efficacy of our method.
AB - An improved method for driving a system into a desired distribution, for example, the Gibbs-Boltzmann distribution, is proposed, which makes use of an artificial relaxation process. The standard techniques for achieving the Gibbs-Boltzmann distribution involve numerical simulations under the detailed balance condition. In contrast, in the present study we formulate the Langevin dynamics, for which the corresponding Fokker-Planck operator includes an asymmetric component violating the detailed balance condition. This leads to shifts in the eigenvalues and results in the acceleration of the relaxation toward the steady state. The numerical implementation demonstrates faster convergence and shorter correlation time, and the technique of biased event sampling, Nemoto-Sasa theory, further highlights the efficacy of our method.
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U2 - 10.1103/PhysRevE.92.012105
DO - 10.1103/PhysRevE.92.012105
M3 - Article
AN - SCOPUS:84937001518
SN - 2470-0045
VL - 92
JO - Physical Review E
JF - Physical Review E
IS - 1
M1 - 012105
ER -