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Generalized dynamical thermostating technique
Author(s) -
Brian B. Laird,
Benedict Leimkuhler
Publication year - 2003
Publication title -
physical review. e, statistical physics, plasmas, fluids, and related interdisciplinary topics
Language(s) - English
Resource type - Journals
eISSN - 1095-3787
pISSN - 1063-651X
DOI - 10.1103/physreve.68.016704
Subject(s) - harmonic oscillator , thermostat , hamiltonian (control theory) , dynamical billiards , physics , ergodicity , symplectic geometry , hamiltonian system , classical mechanics , symplectic integrator , hamiltonian mechanics , statistical physics , quantum mechanics , mathematical physics , mathematical analysis , mathematics , thermodynamics , phase space , integrator , mathematical optimization , voltage
We demonstrate that the Nosé method for constant-temperature molecular-dynamics simulation [Mol. Phys. 52, 255 (1984)] can be substantially generalized by the addition of auxiliary variables to encompass an infinite variety of Hamiltonian thermostats. Such thermostats can be used to enhance ergodicity in systems, such as the one-dimensional harmonic oscillator or certain molecular systems, for which the standard Nosé-Hoover methods fail to reproduce converged canonical distributions. In this respect the method is similar in spirit to the method of Nosé-Hoover chains, but is both more general and Hamiltonian in structure (which allows for the use of efficient symplectic integration schemes). In particular, we show that, within the generalized Nosé formalism outlined herein, any Hamiltonian system can be thermostated with any other, including a copy of itself. This gives one an enormous flexibility in choosing the form of the thermostating bath. Numerical experiments are included in which a harmonic oscillator is thermostated with a collection of noninteracting harmonic oscillators as well as by a soft billiard system.

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