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arXiv 2404.02480cond-mat.stat-mech
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谐振子势阱中具有随机驱动中心的非相互作用粒子

Noninteracting particles in a harmonic trap with a stochastically driven center

Sanjib Sabhapandit, Satya N. Majumdar

AI总结:

本文研究谐振子势阱中心受随机驱动时非相互作用粒子系统的非平衡稳态,证明动力学可自发产生粒子位置间的强关联,并利用条件独立同分布结构解析计算多种统计量。

摘要:

我们研究一维直线上 $N$ 个非相互作用粒子在谐振子势阱 $U(x)=μ\igl[x-z(t)\igr]^2/2$ 中的系统,其中势阱中心 $z(t)$ 经历有界随机调制。我们证明这种随机调制将系统驱动到一个非平衡稳态,在该稳态中粒子位置的联合分布不可因式分解。这表明粒子位置之间存在强关联,这些关联并非内禀存在,而是由动力学本身产生的。此外,我们证明该稳态联合分布可以被完全刻画,并具有一种特殊的条件独立同分布(CIID)结构。这种特殊结构使我们即使在如此强关联的系统中,也能对任意有界驱动 $z(t)$ 解析计算多个可观测量。这些可观测量包括平均密度分布、粒子位置之间的关联、次序统计量和间隙统计量,以及全计数统计。随后,我们将一般结果应用于两个具体例子:(i)$z(t)$ 表示二分电报噪声,(ii)$z(t)$ 表示 Ornstein-Uhlenbeck 过程。我们的解析预测在数值模拟中得到了验证,结果高度吻合。

英文摘要:

We study a system of $N$ noninteracting particles on a line in the presence of a harmonic trap $U(x)=μ\bigl[x-z(t)\bigr]^2/2$, where the trap center $z(t)$ undergoes a bounded stochastic modulation. We show that this stochastic modulation drives the system into a nonequilibrium stationary state, where the joint distribution of the positions of the particles is not factorizable. This indicates strong correlations between the positions of the particles that are not inbuilt, but rather get generated by the dynamics itself. Moreover, we show that the stationary joint distribution can be fully characterized and has a special conditionally independent and identically distributed (CIID) structure. This special structure allows us to compute several observables analytically even in such a strongly correlated system, for an arbitrary bounded drive $z(t)$. These observables include the average density profile, the correlations between particle positions, the order and gap statistics, as well as the full counting statistics. We then apply our general results to two specific examples where (i) $z(t)$ represents a dichotomous telegraphic noise, and (ii) $z(t)$ represents an Ornstein-Uhlenbeck process. Our analytical predictions are verified in numerical simulations, finding excellent agreement.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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