abstract
The early days of quantum mechanics were characterised by debates over the applicability of established classical concepts, such as position and momentum, to the new formulation of mechanics. The issues became quite distinct in the protracted exchange between A. Einstein and N. Bohr, culminating in the paper of Einstein, Podolsky and Rosen (EPR) in 1935 [1]. Bohr, in his response to this paper, [2] expanded upon his concept of complementarity and showed that the EPR argument did not establish the incompleteness of quantum mechanics, as EPR had claimed, but rather highlighted the inapplicability of classical modes of description in the quantum domain. A. Einstein, however, did not accept this position and the two sides of the debate remained unreconciled, while most physicists generally believed that N. Bohr’s argument carried the day.
Thus the matter rested until 1964 when J.S. Bell opened up the possibility of directly testing the consequences of the EPR premises. We will discuss the EPR argument and the analysis of Bell in the context of correlated photon states.
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Walls, D., Milburn, G.J. (2008). Bells Inequalities in Quantum Optics. In: Walls, D., Milburn, G.J. (eds) Quantum Optics. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-540-28574-8_13
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DOI: https://doi.org/10.1007/978-3-540-28574-8_13
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