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arXiv quant-ph/0310081quant-ph
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“Which-Way”实验中的测不准关系:如何用弱值直接观测动量传递

The Uncertainty Relation in "Which-Way" Experiments: How to Observe Directly the Momentum Transfer using Weak Values

J. L. Garretson, H. M. Wiseman, D. T. Pope, D. T. Pegg

摘要:

单向测量破坏了双缝干涉图样。玻尔认为,区分两个相距s的狭缝,粒子的动量传递\wp的随机性为h/s。这被接受了60多年,直到Scully,Englert和Walther(SEW)提出了一个方向方案,他们声称,不需要动量转移。Storey,Tan,Collett和Walls(STCW)反过来证明了一个定理,他们声称,表明玻尔是正确的。这项工作的审查和扩展最近的建议[怀斯曼,物理学快报。A 311,285(2003)]使用动量转移的弱值概率分布P_wv(\wp)来解决该问题。证明了P_wv(\wp)必须大于h/6s.然而,它的矩仍然可以为零,因为P_wv(\wp)不一定是正定的。尽管如此,它还是可以用经典物理学家可以理解的方式来测量的。我们引入了一个新的度量P_wv(\wp)的扩展:单位置信区间的一半,并推测它永远不会小于h/4s。对于无限窄缝的理想化例子,除非使用切趾处理,否则P_wv(\wp)和动量分布的矩是不确定的。我们表明,通过考虑连续平滑的初始波函数,连续更多的时刻的P_wv(\wp)和动量分布变得明确。在这个例子中,P_wv(\wp)的矩为零,这些矩等于动量分布的矩的变化。我们证明了这种关系的计划,其中的时刻P_wv(\wp)是非零的,但只有前两个时刻。我们还比较了这些时刻的其他两个动量转移分布和\hat{p}_f - \hat{p}_i。我们发现所有这些都是一致的,但同样只是前两个时刻。

英文摘要:

A which-way measurement destroys the twin-slit interference pattern. Bohr argued that distinguishing between two slits a distance s apart gives the particle a random momentum transfer \wp of order h/s. This was accepted for more than 60 years, until Scully, Englert and Walther (SEW) proposed a which-way scheme that, they claimed, entailed no momentum transfer. Storey, Tan, Collett and Walls (STCW) in turn proved a theorem that, they claimed, showed that Bohr was right. This work reviews and extends a recent proposal [Wiseman, Phys. Lett. A 311, 285 (2003)] to resolve the issue using a weak-valued probability distribution for momentum transfer, P_wv(\wp). We show that P_wv(\wp) must be wider than h/6s. However, its moments can still be zero because P_wv(\wp) is not necessarily positive definite. Nevertheless, it is measurable in a way understandable to a classical physicist. We introduce a new measure of spread for P_wv(\wp): half of the unit-confidence interval, and conjecture that it is never less than h/4s. For an idealized example with infinitely narrow slits, the moments of P_wv(\wp) and of the momentum distributions are undefined unless a process of apodization is used. We show that by considering successively smoother initial wave functions, successively more moments of both P_wv(\wp) and the momentum distributions become defined. For this example the moments of P_wv(\wp) are zero, and these are equal to the changes in the moments of the momentum distribution. We prove that this relation holds for schemes in which the moments of P_wv(\wp) are non-zero, but only for the first two moments. We also compare these moments to those of two other momentum-transfer distributions and \hat{p}_f-\hat{p}_i. We find agreement between all of these, but again only for the first two moments.

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