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Semiclassical Time Evolution of the Reduced Density Matrix and Dynamically Assisted Generation of Entanglement for Bipartite Quantum Systems

机译:简化的密度矩阵的半经典时间演化和二元量子系统的动态纠缠生成

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摘要

Two particles, initially in a product state, become entangled when they come together and start to interact. Using semiclassical methods, we calculate the time evolution of the corresponding reduced density matrix p_1, obtained by integrating out the degrees of freedom of one of the particles. We find that entanglement generation sensitively depends (ⅰ) on the interaction potential, especially on its strength and range, and (ⅱ) on the nature of the underlying classical dynamics. Under general statistical assumptions, and for short-ranged interaction potentials, we find that p(t) decays exponentially fast in a chaotic environment, whereas it decays only algebraically in a regular system. In the chaotic case, the decay rate is given by the golden rule spreading of one-particle states due to the two-particle coupling, but cannot exceed the system's Lyapunov exponent.
机译:最初处于产品状态的两个粒子在聚在一起并开始相互作用时会发生纠缠。使用半经典方法,我们计算了相应的密度降低矩阵p_1的时间演化,该矩阵通过积分一个粒子的自由度而获得。我们发现纠缠生成敏感地取决于(ⅰ)相互作用的潜力,特别是取决于其强度和范围,并且(ⅱ)取决于基础经典动力学的性质。在一般的统计假设下,对于短距离的相互作用势,我们发现p(t)在混沌环境中呈指数衰减,而在规则系统中仅以代数衰减。在混沌情况下,衰减速率是由于两粒子耦合而由一粒子态的黄金法则扩散给出的,但不能超过系统的李雅普诺夫指数。

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