A unified formulation of the constant temperature molecular dynamics methods

Единая формулировка методов молекулярной динамики при постоянной температуре
Shūichi Nosé
1984-07-01

Haile–Gupta methodHoover methodNosé methodcanonical distributionconstant temperature molecular dynamics
Three recently proposed constant temperature molecular dynamics methods by: (i) Nosé (Mol. Phys., to be published); (ii) Hoover et al. [Phys. Rev. Lett. 48, 1818 (1982)], and Evans and Morriss [Chem. Phys. 77, 63 (1983)]; and (iii) Haile and Gupta [J. Chem. Phys. 79, 3067 (1983)] are examined analytically via calculating the equilibrium distribution functions and comparing them with that of the canonical ensemble. Except for effects due to momentum and angular momentum conservation, method (1) yields the rigorous canonical distribution in both momentum and coordinate space. Method (2) can be made rigorous in coordinate space, and can be derived from method (1) by imposing a specific constraint. Method (3) is not rigorous and gives a deviation of order N−1/2 from the canonical distribution (N the number of particles). The results for the constant temperature–constant pressure ensemble are similar to the canonical ensemble case.
1
Method (i) (Nosé) yields the rigorous canonical distribution in both momentum and coordinate space, except for momentum and angular momentum conservation effects.
2
Method (ii) (Hoover et al. / Evans and Morriss) can be made rigorous in coordinate space and is derivable from method (i) by imposing a specific constraint.
3
Method (iii) (Haile and Gupta) is not rigorous and produces a deviation from the canonical distribution of order N^{-1/2}, where N is particle number.
4
The analysis of constant temperature–constant pressure ensembles produces results similar to those for the canonical ensemble.

Constant-temperature molecular dynamics methods (Nosé, Hoover–Evans–Morriss, Haile–Gupta) and their ensembles

Comparison of equilibrium distribution functions (rigorosity relative to the canonical ensemble) and deviations arising from momentum/angular-momentum conservation and finite-size (order N−1/2) effects, including extension to constant-temperature–constant-pressure ensemble

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1984-07-01
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Shūichi Nosé
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