Bell inequalities and hidden variables over all possible paths in a quantum system
Warren Leffler

TL;DR
This paper introduces a model combining Feynman's path integral formulation with Deutsch's particle interaction to replicate quantum mechanics predictions, challenge Bell's assumptions, and incorporate hidden variables over all possible paths.
Contribution
It develops a novel system that reproduces quantum predictions using all possible paths as hidden variables, bypassing Bell's inequality constraints.
Findings
Replicates quantum mechanics predictions
Contains all possible paths as hidden variables
Challenges Bell's inequality assumptions
Abstract
Bell's theorem rests on the following fundamental condition for a local system: P(a,b|alpha, beta, lambda)= P(a|alpha, lambda)P(b|beta, lambda). Here a and b are the outcomes respectively for measurements alpha on one side, and beta on the other, of an experiment involving two entangled particles traveling in opposite directions from a source. The parameter lambda (the set of "hidden variables") represents a more complete description of the joint state of the two particles. Because of lambda, the joint probability of detection is now dependent only on lambda and the local measurement setting of alpha; similarly for the other side and the setting beta. From this equation John Bell derived a simple inequality that is violated by the predictions of quantum mechanics, which is generally taken to imply that quantum mechanics is a nonlocal theory. But, by combining Richard Feynman's…
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Taxonomy
TopicsQuantum Mechanics and Applications · Quantum Information and Cryptography · Philosophy and History of Science
