Violation of Bell's Inequality in the Clauser-Horne-Shimony-Holt Form with Entangled Quantum States Revisited

• URL: http://arxiv.org/abs/2302.14046v2
• Date: Wed, 1 May 2024 16:16:03 GMT
• Title: Violation of Bell's Inequality in the Clauser-Horne-Shimony-Holt Form with Entangled Quantum States Revisited
• Authors: Carlo Cafaro, Christian Corda, Philip Cairns, Ayhan Bingolbali,
• Abstract summary: We revisit the violation of Bell's inequality in the Clauser-Horne-Shimony-Holt form with entangled quantum states. We show how the extent of this violation depends both on the orientation of the polarizers and the degree of entanglement of the quantum states.
• Score: 0.0
• License: http://creativecommons.org/licenses/by/4.0/
• Abstract: Scientific imagination and experimental ingenuity are at the heart of physics. One of the most known instances where this interplay between theory (i.e., foundations) and experiments (i.e., technology) occurs is in the discussion of Bell's inequalities. In this paper, we present a revisitation of the violation of Bell's inequality in the Clauser-Horne-Shimony-Holt (CHSH) form with entangled quantum states. First, we begin with a discussion of the 1935 Einstein-Podolski-Rosen (EPR) paradox (i.e., incompleteness of quantum mechanics) that emerges from putting the emphasis on Einstein's locality and the absolute character of physical phenomena. Second, we discuss Bell's 1971 derivation of the 1969 CHSH form of the original 1964 Bell inequality in the context of a realistic local hidden-variable theory (RLHVT). Third, identifying the quantum-mechanical spin correlation coefficient with the RLHVT one, we follow Gisin's 1991 analysis to show that quantum mechanics violates Bell's inequality when systems are in entangled quantum states. For pedagogical purposes, we show how the extent of this violation depends both on the orientation of the polarizers and the degree of entanglement of the quantum states. Fourth, we discuss the basics of the experimental verification of Bell's inequality in an actual laboratory as presented in the original 1982 Aspect-Grangier-Roger (AGR) experiment. Finally, we provide an outline of some essential take home messages from this wonderful example of physics at its best.

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