Kinetic moments method for the canonical ensemble distribution
Simultaneous integral control of the kinetic energy 〈 K〉 and its fluctuation 〈 K 2〉 - 〈 K〉 2 gives an extended phase-space distribution consistent with Gibbs' canonical one. This generalization of the Nosé-Hoover approach to thermostatting is the simplest time-reversible scheme to exhibit ergod...
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Published in: | Physics letters. A Vol. 211; no. 5; pp. 253 - 257 |
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Main Authors: | , |
Format: | Journal Article |
Language: | English |
Published: |
Elsevier B.V
26-02-1996
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Online Access: | Get full text |
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Summary: | Simultaneous integral control of the kinetic energy 〈
K〉 and its fluctuation 〈
K
2〉 - 〈
K〉
2 gives an extended phase-space distribution consistent with Gibbs' canonical one. This generalization of the Nosé-Hoover approach to thermostatting is the simplest time-reversible scheme to exhibit ergodicity for the one-dimensional harmonic oscillator. It is also applicable to equilibrium and nonequilibrium many-body simulations. |
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ISSN: | 0375-9601 1873-2429 |
DOI: | 10.1016/0375-9601(95)00973-6 |