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HEISENBERG UNCERTAINTY RELATION REVISITED-UNIVERSALITY OF ROBERTSON'S RELATION

机译:修改后的海森堡不确定性关系-罗伯逊关系的普遍性

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摘要

It is shown that all the known uncertainty relations are the secondary consequences of Robertson's relation. The basic idea is to use the Heisenberg picture so that the time development of quantum mechanical operators incorporate the effects of the measurement interaction. A suitable use of triangle inequalities then gives rise to various forms of uncertainty relations. The assumptions of unbiased measurement and unbiased disturbance are important to simplify the resulting uncertainty relations and to give the familiar uncertainty relations, such as a naive Heisenberg error-disturbance relation. These simplified uncertainty relations are however, valid only conditionally. Quite independently of uncertainty relations, it is shown that the notion of precise measurement is incompatible with the assumptions of unbiased measurement and unbiased disturbance. We can thus naturally understand the failure of the naive Heisenberg's error-disturbance relation, as was demonstrated by the recent spin measurement by Erhart et al.
机译:结果表明,所有已知的不确定性关系都是罗伯逊关系的次要结果。基本思想是使用海森堡图像,以便量子力学算子的时间发展吸收测量相互作用的影响。三角形不等式的适当使用会引起各种形式的不确定性关系。无偏测量和无偏扰动的假设对于简化由此产生的不确定性关系并给出熟悉的不确定性关系(例如幼稚的海森堡误差-干扰关系)非常重要。但是,这些简化的不确定性关系仅在有条件的情况下有效。完全独立于不确定性关系,它表明精确测量的概念与无偏测量和无偏干扰的假设是不相容的。因此,我们自然可以理解朴素的海森堡误差与干扰关系的失败,正如Erhart等人最近的自旋测量所证明的那样。

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