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arXiv 2003.09351cond-mat.stat-mechnlin.CD
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含时势阱中粒子的混沌扩散

Chaotic diffusion for particles moving in a time dependent potential well

Edson D. Leonel, Celia Mayumi Kuwana, Makoto Yoshida, Juliano Antonio de Oliveira

摘要:

用两种不同的方法描述了在含时势阱中运动的粒子的混沌扩散:(i)通过描述动力学的映射的直接演化;(ii)通过扩散方程的解。扩散粒子的动力学是通过使用一个二维的,非线性区域保持映射的变量能量和时间。系统的相空间是混合的,包含混沌、周期区域和限制混沌粒子扩散的不变生成曲线。粒子系综的混沌演化被视为粒子的随机运动,因此由扩散方程描述。边界条件要求粒子不能穿过作为扩散上边界的不变生成曲线,也不能穿过作为粒子从时移势阱逃逸能量的最低能量域。扩散系数通过映射方程确定,而扩散方程的解析解给出了在特定时间找到具有特定能量的给定粒子的概率。动量的概率定性描述的行为的平均能量通过数值模拟,这是研究无论是作为一个函数的时间,以及一些控制参数的问题。

英文摘要:

The chaotic diffusion for particles moving in a time dependent potential well is described by using two different procedures: (i) via direct evolution of the mapping describing the dynamics and ; (ii) by the solution of the diffusion equation. The dynamic of the diffusing particles is made by the use of a two dimensional, nonlinear area preserving map for the variables energy and time. The phase space of the system is mixed containing both chaos, periodic regions and invariant spanning curves limiting the diffusion of the chaotic particles. The chaotic evolution for an ensemble of particles is treated as random particles motion and hence described by the diffusion equation. The boundary conditions impose that the particles can not cross the invariant spanning curves, serving as upper boundary for the diffusion, nor the lowest energy domain that is the energy the particles escape from the time moving potential well. The diffusion coefficient is determined via the equation of the mapping while the analytical solution of the diffusion equation gives the probability to find a given particle with a certain energy at a specific time. The momenta of the probability describe qualitatively the behavior of the average energy obtained by numerical simulation, which is investigated either as a function of the time as well as some of the control parameters of the problem.

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