The EPR Paradox and the quantum correlations described by Bell's Inequality theorem, are explained as arising from the behavior of entities that manifest only a single bit of information, such as noisy, band-limited, polarized coins.
It is almost universally supposed, that “Quantum Correlations”, as discussed in connection with Bell’s Inequality Theorem, cannot be produced by any classical, macroscopic system. Nevertheless, this paper demonstrates the actual construction of just such a system. It then discusses why this peculiar type of classical system, unlike any other, behaves in this “weird” fashion. The reason illuminates the Physics Community’s profound misunderstanding of exactly what a single, classical “bit” is, in the context of Shannon’s Information Theory, and the resulting misinterpretation of the Heisenberg Uncertainty Principle and the EPR paradox.
The EPR paradox was caused by the provision that quantum variables must have pre-existing values. This type of "hidden property realism" was later falsified by Bell's Theorem. Accordingly, the physical basis for action-at-a-distance between entangled quanta was removed. Yet, modern interpretations present Bell's inequality as a Locality Criterion, as if Bell violations can only happen at the quantum level, and only with remote interactions. This is a questionable practice, considering that classical joint measurements also violate such inequalities for mutually exclusive wave properties. In particular, consecutive measurements of polarization produce the same coefficients of correlation as parallel measurements with entangled quanta, yet they are explicitly local. Furthermore, it is possible to combine parallel and consecutive measurements of Type I polarization-entangled photons in a single experiment, conclusively showing that quantum Bell violations can be local. Surprisingly, classical phenomena also require nonlocal interpretations if pre-existing properties are taken for granted. Hence, the solution is to reject the models with pre-existing properties for both classical and quantum wave-like phenomena.