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具有随机动力学的长程相互作用系统中的缓慢松弛。

Slow relaxation in long-range interacting systems with stochastic dynamics.

机构信息

Physics of Complex Systems, Weizmann Institute of Science, Rehovot 76100, Israel.

出版信息

Phys Rev Lett. 2010 Jul 23;105(4):040602. doi: 10.1103/PhysRevLett.105.040602.

Abstract

Quasistationary states are long-lived nonequilibrium states, observed in some systems with long-range interactions under deterministic Hamiltonian evolution. These intriguing non-Boltzmann states relax to equilibrium over times which diverge algebraically with the system size. To test the robustness of this phenomenon to nondeterministic dynamical processes, we have generalized the paradigmatic model exhibiting such a behavior, the Hamiltonian mean-field model, to include energy-conserving stochastic processes. Analysis, based on the Boltzmann equation, a scaling approach, and numerical studies, demonstrates that in the long time limit the system relaxes to the equilibrium state on time scales which do not diverge algebraically with the system size. Thus, quasistationarity takes place only as a crossover phenomenon on times determined by the strength of the stochastic process.

摘要

准静态态是长寿命的非平衡态,在某些具有长程相互作用的系统中,在确定性哈密顿演化下被观测到。这些引人入胜的非玻尔兹曼态通过与系统大小呈代数发散的时间来弛豫到平衡。为了测试这种现象对非确定性动力学过程的稳健性,我们已经将表现出这种行为的典范模型,哈密顿平均场模型,推广到包括能量守恒的随机过程。基于玻尔兹曼方程、标度方法和数值研究的分析表明,在长时间限制下,系统在不与系统大小呈代数发散的时间尺度上弛豫到平衡态。因此,准静态态仅作为由随机过程强度决定的时间的交叉现象发生。

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