Spin Theory Based on the Extended Least Action Principle and Information Metrics: Quantization, Entanglement, and Bell Test With Time Delay

Jianhao M. Yang
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Abstract

A theory of electron spin is developed here based on the extended least action principle and assumptions of intrinsic angular momentum of an electron with random orientations. By incorporating appropriate relative entropy for the random orientations of intrinsic angular momentum in the extended least action principle, the theory recovers the quantum formulation of electron spin. The two-level quantization of spin measurement is a natural mathematical consequence instead of a postulate. The formulation of measurement probability when a second Stern-Gerlach apparatus is rotated relative to the first Stern-Gerlach apparatus, and the Schr\"{o}dinger-Pauli equation, are also derived successfully. Furthermore, we provide an intuitive physical model and formulation to explain the entanglement phenomenon between two electron spins. In this model, spin entanglement is the consequence of correlation between the random orientations of the intrinsic angular momenta of the two electrons. Since the orientation is an intrinsic local property of electron, the correlation of orientations can be preserved even when the two electrons are remotely separated. Such a correlation can be manifested without causal effect. Owing to this orientation correlation, the Bell-CHSH inequality is shown to be violated in a Bell test. The standard quantum theory of electron spin can be considered as an ideal approximation of the present theory when certain conditions are taken to the limits. A potential experiment is proposed to test the difference between the present theory and the standard quantum theory. In a typical Bell test that confirms the violation of Bell-CHSH inequality, the theory suggests that by adding a sufficiently large time delay before Bob's measurement, the Bell-CHSH inequality can become non-violated.
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基于扩展最小作用原理和信息度量的自旋理论:量子化、纠缠和有时间延迟的贝尔试验
本文基于扩展最小作用原理和电子固有角动量随机取向假设,提出了电子自旋理论。通过将本征角动量随机取向的适当相对熵纳入扩展最小作用原理,该理论恢复了电子自旋的量子形式。自旋测量的两级量子化是一个自然的数学结果,而不是一个假设。当第二个斯特恩-格拉赫仪器相对于第一个斯特恩-格拉赫仪器旋转时,测量概率的表述以及施尔丁格-保利方程也被成功地推导出来。此外,我们还提供了一个直观的物理模型和公式来解释两个电子自旋之间的纠缠现象。在这个模型中,自旋纠缠是两个电子固有角矩的随机方向之间相关性的结果。由于这种方位相关性,贝尔-CHSH 不等式在贝尔试验中被证明是违反的。当某些条件达到极限时,电子自旋的标准量子理论可被视为本理论的理想近似。我们提出了一个潜在的实验来检验本理论与标准量子理论之间的差异。在证实违反贝尔-CHSH 不等式的非典型贝尔测试中,该理论认为,在鲍勃的测量之前添加足够大的时间延迟,贝尔-CHSH 不等式就可以变得不违反。
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