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Quantum arrival and dwell times via idealized clocks

机译:通过理想化时钟实现量子到达和停留时间

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摘要

A number of approaches to the problem of defining arrival- and dwell-time probabilities in quantum theory makes use of idealized models of clocks. An interesting question is the extent to which the probabilities obtained in this way are related to standard semiclassical results. In this paper, we explore this question using a reasonably general clock model, solved using path-integral methods. We find that, in the weak-coupling regime, where the energy of the clock is much less than the energy of the particle it is measuring, the probability for the clock pointer can be expressed in terms of the probability current in the case of arrival times, and the dwell-time operator in the case of dwell times, the expected semiclassical results. In the regime of strong system-clock coupling, we find that the arrival-time probability is proportional to the kinetic-energy density, consistent with an earlier model involving a complex potential. We argue that, properly normalized, this may be the generically expected result in this regime. We show that these conclusions are largely independent of the form of the clock Hamiltonian.
机译:解决量子理论中到达和驻留时间概率问题的许多方法都使用了理想的时钟模型。一个有趣的问题是,以这种方式获得的概率在多大程度上与标准半经典结果相关。在本文中,我们使用合理的通用时钟模型探索这个问题,并使用路径积分方法解决。我们发现,在弱耦合状态下,时钟的能量远小于其正在测量的粒子的能量,可以用到达时电流的概率来表示时钟指针的概率。时间,以及在停留时间的情况下的停留时间运算符,则预期的半经典结果。在强系统时钟耦合机制中,我们发现到达时间概率与动能密度成正比,这与涉及复杂电势的早期模型是一致的。我们认为,适当地归一化,这可能是该政权普遍预期的结果。我们表明,这些结论在很大程度上与时钟哈密顿量的形式无关。

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