Kupczynski Marian
Department of Computer Science and Engineering, University of Quebec in Outaouais (UQO), Case Postale 1250, Succursale Hull, Gatineau, QC J8X 3X7, Canada.
Entropy (Basel). 2023 Feb 2;25(2):280. doi: 10.3390/e25020280.
A violation of Bell-CHSH inequalities does not justify speculations about quantum non-locality, conspiracy and retro-causation. Such speculations are rooted in a belief that setting dependence of hidden variables in a probabilistic model (called a violation of (MI)) would mean a violation of experimenters' freedom of choice. This belief is unfounded because it is based on a questionable use of Bayes Theorem and on incorrect causal interpretation of conditional probabilities. In Bell-local realistic model, hidden variables describe only photonic beams created by a source, thus they cannot depend on randomly chosen experimental settings. However, if hidden variables describing measuring instruments are correctly incorporated into a contextual probabilistic model a violation of inequalities and an apparent violation of no-signaling reported in Bell tests can be explained without evoking quantum non-locality. Therefore, for us, a violation of Bell-CHSH inequalities proves only that hidden variables have to depend on settings confirming contextual character of quantum observables and an active role played by measuring instruments. Bell thought that he had to choose between non-locality and the violation of experimenters' freedom of choice. From two bad choices he chose non-locality. Today he would probably choose the violation of MI understood as .
违反贝尔-CHSH不等式并不能为关于量子非局域性、阴谋论和逆因果关系的推测提供依据。此类推测源于一种信念,即概率模型中隐藏变量的设定依赖性(称为违反(MI))将意味着违反实验者的选择自由。这种信念是没有根据的,因为它基于对贝叶斯定理的不当运用以及对条件概率的错误因果解释。在贝尔局域实在模型中,隐藏变量仅描述由源产生的光子束,因此它们不能依赖于随机选择的实验设定。然而,如果将描述测量仪器的隐藏变量正确纳入情境概率模型,那么在不引发量子非局域性的情况下,就可以解释贝尔测试中报告的不等式违反和明显的无信号违反现象。因此,对我们而言,违反贝尔-CHSH不等式仅证明隐藏变量必须依赖于设定,这证实了量子可观测量的情境特征以及测量仪器所起的积极作用。贝尔认为他必须在非局域性和违反实验者的选择自由之间做出选择。在两个糟糕的选择中,他选择了非局域性。如今他可能会选择将违反MI理解为 。