1984
DOI: 10.1080/00268978400101201
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A molecular dynamics method for simulations in the canonical ensemble

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Cited by 8,355 publications
(3,930 citation statements)
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References 17 publications
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“…The Nosé-Hoover thermostat 39,40 was applied to control the temperature at 298 K, while the normal pressure was kept at 1 bar using the semi-isotropic form of the Parrinello-Rahman barostat 41 . The interfacial systems were constructed by first equilibrating two separate boxes containing the water and organic liquids with the same cross-sectional dimensions.…”
Section: Simulation Methodsmentioning
confidence: 99%
“…The Nosé-Hoover thermostat 39,40 was applied to control the temperature at 298 K, while the normal pressure was kept at 1 bar using the semi-isotropic form of the Parrinello-Rahman barostat 41 . The interfacial systems were constructed by first equilibrating two separate boxes containing the water and organic liquids with the same cross-sectional dimensions.…”
Section: Simulation Methodsmentioning
confidence: 99%
“…For completeness, a detailed simulation protocol is given in Table I. The MD-simulations are carried out in the NPT ensemble using the Nosé-Hoover thermostat [51,52] and the Rahman-Parrinello barostat [53,54] with coupling times τ T = 1.5 ps and τ p = 2.5 ps (assuming an isothermal compressibility of χ T = 4.5 10 −5 bar −1 ), respectively. The electrostatic interactions are treated in the "full potential" approach by the smooth particle mesh Ewald summation [55] with a real space cutoff of 0.9 nm and a mesh spacing of approximately 0.12 nm and 4th order interpolation.…”
Section: A MD Simulation Detailsmentioning
confidence: 99%
“…(6), is employed to obtain the required ensemble. Here, the detailed balance condition is described in terms of the amount of stochastic flow as follows:…”
Section: A Markov Chain Monte Carlo Methods With the Weight Allocationmentioning
confidence: 99%
“…To see usefulness of the Suwa-Todo algorithm for the replica-permutation method, we per- the Gaussian constraint method [4,5] to avoid the problem of non-ergodicity in the Nosé-Hoover thermostat [6][7][8] for the non-interacting particle system. The trajectory data were stored every 10.0 fs.…”
Section: A Asymmetric Double-well Potential Energymentioning
confidence: 99%
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