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腔量子电动力学中原子 - 光子相互作用的混沌与跃迁

Chaos and flights in the atom-photon interaction in cavity QED.

作者信息

Prants S V, Edelman M, Zaslavsky G M

机构信息

Laboratory of Nonlinear Dynamical Systems, Viktor Il'ichev Pacific Oceanological Institute of the Russian Academy of Sciences, 2690041 Vladivostok, Russia.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2002 Oct;66(4 Pt 2):046222. doi: 10.1103/PhysRevE.66.046222. Epub 2002 Oct 30.

Abstract

We study dynamics of the atom-photon interaction in cavity quantum electrodynamics, considering a cold two-level atom in a single-mode high-finesse standing-wave cavity as a nonlinear Hamiltonian system with three coupled degrees of freedom: translational, internal atomic, and the field. The system proves to have different types of motion including Lévy flights and chaotic walkings of an atom in a cavity. The corresponding equations of motion for expectation values of the atom and field variables have two characteristic time scales: fast Rabi oscillations of the internal atomic and field quantities and slow translational oscillations of the center of the atom mass. It is shown that the translational motion, related to the atom recoils, is governed by an equation of a parametric nonlinear pendulum with a frequency modulated by the Rabi oscillations. This type of dynamics is chaotic with some width of the stochastic layer that is estimated analytically. The width is fairly small for realistic values of the control parameters, the normalized detuning delta and atomic recoil frequency alpha. We consider the Poincaré sections of the dynamics, compute the Lyapunov exponents, and find a range of the detuning, |delta| less, similar 3, where chaos is prominent. It is demonstrated how the atom-photon dynamics with a given value of alpha depends on the values of delta and initial conditions. Two types of Lévy flights, one corresponding to the ballistic motion of the atom and the other corresponding to small oscillations in a potential well, are found. These flights influence statistical properties of the atom-photon interaction such as distribution of Poincaré recurrences and moments of the atom position x. The simulation shows different regimes of motion, from slightly abnormal diffusion with <x(2)> approximately tau(1.13) at delta=1.2 to a superdiffusion with <x(2)> approximately tau(2.2) at delta=1.92 that corresponds to a superballistic motion of the atom with an acceleration. The obtained results can be used to find new ways to manipulate atoms, to cool and trap them by adjusting the detuning delta.

摘要

我们研究腔量子电动力学中原子 - 光子相互作用的动力学,将单模高精细度驻波腔中的冷二能级原子视为具有三个耦合自由度的非线性哈密顿系统:平移自由度、原子内部自由度和场自由度。该系统被证明具有不同类型的运动,包括腔中原子的 Lévy 飞行和混沌行走。原子和场变量期望值的相应运动方程有两个特征时间尺度:原子内部和场量的快速拉比振荡以及原子质心的缓慢平移振荡。结果表明,与原子反冲相关的平移运动由一个参数非线性摆方程支配,其频率由拉比振荡调制。这种动力学类型是混沌的,具有一个通过解析估计的随机层宽度。对于控制参数的实际值,即归一化失谐量δ和原子反冲频率α,该宽度相当小。我们考虑动力学的庞加莱截面,计算李雅普诺夫指数,并找到失谐量的一个范围,即|δ| < 约 3,其中混沌现象显著。展示了具有给定α值的原子 - 光子动力学如何依赖于δ值和初始条件。发现了两种类型的 Lévy 飞行,一种对应于原子的弹道运动,另一种对应于势阱中的小振荡。这些飞行影响原子 - 光子相互作用的统计性质,例如庞加莱回归的分布和原子位置 x 的矩。模拟显示了不同的运动状态,从在δ = 1.2 时<x²> ≈ τ¹·¹³ 的轻微异常扩散到在δ = 1.92 时<x²> ≈ τ²·² 的超扩散,后者对应于原子的加速超弹道运动。所得结果可用于寻找操纵原子的新方法,通过调整失谐量δ来冷却和捕获原子。

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