Bell’s Inequality

J. Tooker
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Abstract

We show that when spin eigenfunctions are not fully orthonormal, Bell's inequality does allow local hidden variables. In the limit where spin eigenfunctions are Dirac orthonormal, we recover a significant extremal case. The new calculation gives a possible accounting for $\alpha_{\mathrm{MCM}}-\alpha_{\mathrm{QED}}$.
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我们证明了当自旋本征函数不完全正交时,贝尔不等式允许存在局部隐变量。在自旋本征函数是狄拉克标准正交的极限下,我们恢复了一个重要的极端情况。新的计算给出了$\alpha_{\mathrm{MCM}}-\alpha_{\mathrm{QED}}$的可能计算方法。
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