Use of the weighted histogram analysis method for the analysis of simulated and parallel tempering simulations

被引:389
作者
Chodera, John D. [1 ]
Swope, William C.
Pitera, Jed W.
Seok, Chaok
Dill, Ken A.
机构
[1] Univ Calif San Francisco, Grad Grp Biophys, San Francisco, CA 94143 USA
[2] Univ Calif San Francisco, Dept Pharmaceut Chem, San Francisco, CA 94143 USA
[3] IBM Corp, Almaden Res Ctr, San Jose, CA 95120 USA
[4] Seoul Natl Univ, Coll Nat Sci, Dept Chem, Seoul 151747, South Korea
关键词
D O I
10.1021/ct0502864
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
The growing adoption of generalized-ensemble algorithms for biomolecular simulation has resulted in a resurgence in the use of the weighted histogram analysis method (WHAM) to make use of all data generated by these simulations. Unfortunately, the original presentation of WHAM by Kumar et al. is not directly applicable to data generated by these methods. WHAM was originally formulated to combine data from independent samplings of the canonical ensemble, whereas many generalized-ensemble algorithms sample from mixtures of canonical ensembles at different temperatures. Sorting configurations generated from a parallel tempering simulation by temperature obscures the temporal correlation in the data and results in an improper treatment of the statistical uncertainties used in constructing the estimate of the density of states. Here we present variants of WHAM, STWHAM and PTWHAM, derived with the same set of assumptions, that can be directly applied to several generalized ensemble algorithms, including simulated tempering, parallel tempering (better known as replica-exchange among temperatures), and replica-exchange simulated tempering. We present methods that explicitly capture the considerable temporal correlation in sequentially generated configurations using autocorrelation analysis. This allows estimation of the statistical uncertainty in WHAM estimates of expectations for the canonical ensemble. We test the method with a one-dimensional model system and then apply it to the estimation of potentials of mean force from parallel tempering simulations of the alanine dipeptide in both implicit and explicit solvent.
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页码:26 / 41
页数:16
相关论文
共 46 条
[1]  
[Anonymous], 1997, Computer Simulation of Biomolecular Systems: Theoretical and Experimental Applications
[2]   MOLECULAR-DYNAMICS WITH COUPLING TO AN EXTERNAL BATH [J].
BERENDSEN, HJC ;
POSTMA, JPM ;
VANGUNSTEREN, WF ;
DINOLA, A ;
HAAK, JR .
JOURNAL OF CHEMICAL PHYSICS, 1984, 81 (08) :3684-3690
[3]   MULTICANONICAL ALGORITHMS FOR 1ST ORDER PHASE-TRANSITIONS [J].
BERG, BA ;
NEUHAUS, T .
PHYSICS LETTERS B, 1991, 267 (02) :249-253
[4]   MULTICANONICAL ENSEMBLE - A NEW APPROACH TO SIMULATE 1ST-ORDER PHASE-TRANSITIONS [J].
BERG, BA ;
NEUHAUS, T .
PHYSICAL REVIEW LETTERS, 1992, 68 (01) :9-12
[5]  
Case D. A., 2002, AMBER7
[6]  
CASELLA G, 1998, STAT INFERENCE
[7]  
Cowan G., 1998, Statistical Data Analysis
[8]   PARTICLE MESH EWALD - AN N.LOG(N) METHOD FOR EWALD SUMS IN LARGE SYSTEMS [J].
DARDEN, T ;
YORK, D ;
PEDERSEN, L .
JOURNAL OF CHEMICAL PHYSICS, 1993, 98 (12) :10089-10092
[9]   The loop algorithm [J].
Evertz, HG .
ADVANCES IN PHYSICS, 2003, 52 (01) :1-66
[10]   OPTIMIZED MONTE-CARLO DATA-ANALYSIS [J].
FERRENBERG, AM ;
SWENDSEN, RH .
PHYSICAL REVIEW LETTERS, 1989, 63 (12) :1195-1198