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Thermal quantum transition-path-time distributions, time averages, and quantum tunneling times

机译:热量子转换 - 路径时间分布,时间平均值和量子隧道时间

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The transition-path-time distribution is formalized for quantum systems and applied to a number of examples. Using a symmetrized thermal density, transition times are studied for the free particle, a δ-function potential, a square-barrier potential, and symmetric-double-well dynamics at very low temperature. These studies exemplify extreme nonlocality for motion in δ-function potentials, vanishing tunneling times for the square-barrier potential, and varying transit times in the symmetric-double-well potential. In all cases, there are regions where the longer the distance traversed, the shorter the mean transit time is. For the thermal density correlation functions studied here, the Hartman effect exemplifies itself through the independence of the transit time on the barrier height. However, due to the thermal distribution, the transit time does depend on the barrier width, initially decreasing with increasing width but then increasing again.
机译:转换路径时间分布正式用于量子系统并应用于许多示例。 使用对称的热密度,在非常低温下研究自由粒子,Δ函数电位,方形阻挡电位和对称 - 双孔动力学的转变时间。 这些研究举例说明了在δ函数电位中运动的极端非界面,用于方形屏障电位的隧道延伸时间,并在对称的双阱电位中变化的运输时间。 在所有情况下,有些地区遍历距离越长,平均运输时间越短。 对于这里研究的热密度相关函数,Hartman效果通过在屏障高度上的横向时间的独立性的独立性来实现自身。 然而,由于热分布,运输时间确实取决于阻挡宽度,最初随着宽度的增加而减小,而是再次增加。

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