Genre
- Journal Article
In this paper various extensions of the parallel-tempering algorithm are developed and their properties are analyzed. The algorithms are designed to alleviate quasiergodic sampling in systems which have rough energy landscapes by coupling individual Monte Carlo chains to form a composite chain. As with parallel tempering, the procedures are based upon extending the state space to include parameters to encourage sampling mobility. One of the drawbacks of the parallel-tempering method is the stochastic nature of the Monte Carlo dynamics in the auxiliary variables which extend the state spate. In this work. the possibility of improving the sampling rate by designing deterministic methods of moving through the parameter space is investigated. The methods developed in this article, which are based upon a statistical quenching and heating procedure similar in spirit to simulated annealing, are tested on a simple two-dimensional spin system (xy model) and on a model in vacuo polypeptide system. In the coupled Monte Carlo chain algorithms, we find that the net mobility of the composite chain is determined by the competition between the characteristic time of coupling between adjacent chains and the degree of overlap of their distributions. Extensive studies of all methods are carried out to obtain optimal sampling conditions. In particular, the most efficient parallel-tempering procedure is to attempt to swap configurations after very few Monte Carlo updates of the composite chains. Furthermore, it is demonstrated that, contrary to expectations, the deterministic procedure does not improve the sampling rate over that of parallel tempering.
Univ Toronto, Dept Chem, Chem Phys Theory Grp, Toronto, ON M5S 3H6, Canada.; Opps, SB, Univ Toronto, Dept Chem, Chem Phys Theory Grp, Toronto, ON M5S 3H6, Canada.
COLLEGE PK; ONE PHYSICS ELLIPSE, COLLEGE PK, MD 20740-3844 USA
AMERICAN PHYSICAL SOC
PT: J; CR: *POL CORP, 1990, QUANTA PAR HDB BERG BA, 1991, PHYS LETT B, V267, P249 BERG BA, 1992, INT J MOD PHYS C, V3, P1083 BERG BA, 1992, PHYS REV LETT, V68, P9 BERG BA, 1992, PHYS REV LETT, V69, P2292 BINDER K, 1992, MONTE CARLO SIMULATI FRANTZ DD, 1990, J CHEM PHYS, V93, P2769 GEYER CJ, 1991, COMPUTING SCI STAT, P156 GEYER CJ, 1995, J AM STAT ASSOC, V90, P909 HANSMANN UHE, 1993, J COMPUT CHEM, V14, P1333 HANSMANN UHE, 1997, CHEM PHYS LETT, V281, P140 HAO MH, 1994, J PHYS CHEM-US, V98, P4940 HUKUSHIMA K, 1996, J PHYS SOC JPN, V65, P1604 IFTIMIE R, 2000, J CHEM PHYS, V113, P4852 KERLER W, 1994, PHYS REV E, V50, P4220 KIRKPATRICK S, 1983, SCIENCE, V220, P671 LYUBARTSEV AP, 1992, J CHEM PHYS, V96, P1776 MARINARI E, 1992, EUROPHYS LETT, V19, P451 METROPOLIS N, 1953, J CHEM PHYS, V21, P1087 NEAL RM, UNPUB NEAL RM, 1996, STAT COMPUT, V6, P353 TESI MC, 1996, J STAT PHYS, V82, P155 TORRIE GM, 1977, J COMPUT PHYS, V23, P187 VALLEAU JP, 1977, STAT MECH, P114 VALLEAU JP, 1993, J CHEM PHYS, V99, P4718; NR: 25; TC: 4; J9: PHYS REV E; PN: Part 2; PG: 11; GA: 432ZL
Source type: Electronic(1)
Language
- English
Subjects
- Physics, Mathematical
- FREE-ENERGY
- ALGORITHM
- DISTRIBUTIONS
- Physics, Fluids & Plasmas
- PHASE-TRANSITIONS
- SPIN-GLASS SIMULATIONS