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Nonequilibrium Statistical Mechanics of Systems with Long-Range Interactions: Ubiquity of Core-Halo Distributions

机译:具有远程系统的非平衡统计力学   交互:无处不在的核心 - 光晕分布

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摘要

Systems with long-range (LR) forces, for which the interaction potentialdecays with the interparticle distance with an exponent smaller than thedimensionality of the embedding space, remain an outstanding challenge tostatistical physics. The internal energy of such systems lacks extensivity andadditivity. Although the extensivity can be restored by scaling the interactionpotential with the number of particles, the non-additivity still remains. Lackof additivity leads to inequivalence of statistical ensembles. Before relaxingto thermodynamic equilibrium, isolated systems with LR forces become trapped inout-of-equilibrium quasi-stationary state (qSS), the lifetime of which divergeswith the number of particles. Therefore, in thermodynamic limit LR systems willnot relax to equilibrium. The qSSs are attained through the process ofcollisionless relaxation. Density oscillations lead to particle-waveinteractions and excitation of parametric resonances. The resonant particlesescape from the main cluster to form a tenuous halo. Simultaneously, this coolsdown the core of the distribution and dampens out the oscillations. When allthe oscillations die out the ergodicity is broken and a qSS is born. In thisreport, we will review a theory which allows us to quantitatively predict theparticle distribution in the qSS. The theory is applied to various LRinteracting systems, ranging from plasmas to self-gravitating clusters andkinetic spin models.
机译:具有远距离(LR)力的系统的相互作用势随粒子间距离的衰减而减小,且指数间的差小于包埋空间的维数,这仍然是统计学物理学面临的巨大挑战。这种系统的内部能量缺乏可扩展性和可加性。尽管可通过按粒子数缩放相互作用势来恢复可扩展性,但仍保持非可加性。缺少可加性会导致统计集合的不等式。在放松到热力学平衡之前,具有LR力的孤立系统陷入了非平衡准平稳状态(qSS),其寿命与粒子数不同。因此,在热力学极限下,LR系统将不会松弛到平衡。通过无碰撞松弛过程获得qSS。密度振荡导致粒子波相互作用和参量共振的激发。共振粒子从主簇中逃逸,形成微弱的光环。同时,这可以冷却分配器的核心并抑制振荡。当所有的振荡消失后,遍历性被打破,qSS诞生了。在本报告中,我们将回顾一个理论,该理论使我们能够定量预测qSS中的颗粒分布。该理论适用于各种LR相互作用系统,范围从等离子体到自重团簇和动力学自旋模型。

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