Abstract

This paper intends to show how the fabled violation of Bell’s inequality by the probabilistic specifications of quantum mechanics derives from a mathematical error, an error of neglect. I have no objection to the probabilities specified by quantum theory, nor to the inequality itself as characterized in the formulation of Clauser, Horne, Shimony, and Holt. Designed to assess consequences of Einstein’s principle of local realism, the inequality pertains to a linear combination of four polarization products on the same pair of photons arising in a gedankenexperiment. My assessment displays that in this context, the summands of the relevant CHSH quantity s(λ) inhere four symmetric functional relations which have long been neglected in analytic considerations. Its expectation E[s(λ)] is not the sum of four “marginal” expectations from a joint distribution, as quantum theory explicitly avoids such a specification. Rather, I show that E[s(λ)] has four distinct representations as the sum of three expectations of polarization products plus the expectation of a fourth which is restricted to equal a function value determined by the other three. Analysis using Bruno de Finetti’s fundamental theorem of prevision (FTP) yields only a bound for E(s) within (1.1213,2] , surely not at all as is commonly understood. I exhibit slices of the 4-dimensional polytope of joint P++ probabilities actually motivated by quantum theory at the four stipulated angle settings, as it passes through 3-dimensional space. Bell’s inequality is satisfied everywhere within the convex hull of extreme distributions cohering with quantum theoretic specifications, even while in keeping with local realism. Aspect’s proposed “estimation” of E(s) near to is based on polarization products from different photon pairs that do not have embedded within them the functional relations inhering in the relevant gedankenexperiment. When one actively embeds the restrictions into Aspect’s estimation procedure, it yields an estimate of 1.7667, although this is not and cannot be definitive. While my analysis supports the subjectivist construction of probability as clarifying issues relevant to the interpretation of quantum theory, the error resolved herein is purely mathematical. It pertains to the reconsideration of Bell violation irrespective of one’s attitude toward the meaning of probability.

Highlights

  • As brash as this may sound, claims that probabilistic specifications of quantum mechanics are inconsistent with local realism and defy Bell’s inequality are just plain wrong

  • Designed to assess consequences of Einstein’s principle of local realism, the inequality pertains to a linear combination of four polarization products on the same pair of photons arising in a gedankenexperiment

  • We should recognize and expressly declare that this principle of local realism is based upon a claim that lies outside the bounds of matters addressed by the theory of quantum physics

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Summary

Introduction

As brash as this may sound, claims that probabilistic specifications of quantum mechanics are inconsistent with local realism and defy Bell’s inequality are just plain wrong. The polarizer addressed by photon A is oriented in a variable direction a* in the ( x, y) plane perpendicular to z A It can be set in either of two specific directions designated as a and a′ in the experimental setups we shall consider. Bell’s inequality is relevant to this context in which the two photon polarization directions can be paired at any one of four distinct relative angles, denoted by the parenthetic pairs (a,b) , (a,b′) , (a′,b) , or (a′,b′). As the value p, for example, implies that the pmf vector [ ] P++ , P−− , P+− , P−+ would be p, p,(1− 2 p) 2,(1− 2 p) 2 Another implication of this feature is that the probabilities for the paired detection outcomes depend only on the product of the two measurements. The QM-motivated distribution for the experimental value of the polarization product ( ) ( ) ( ) ( ) ( ) A a* B b* is specified by P A a* B b* =+1 =cos a*,b* and

Lad DOI
The Uncertainty Principle
The Principle of Local Realism and Its Relevance to Bell
Einstein’s Proposal of Hidden Variables Relevant to the Matter
Explicit Construction of s with Hidden Variables
The Mistaken Violation of Bell’s Inequality
A Neglected Functional Dependence
The Realm Matrix of Experimental Quantities
Specifying the Functional Form via Block Four
The Remaining Block of Quantities and Their Realm Components
The Relevance of the Fundamental Theorem of Probability
The Result
Transforming the Expectation Polytope into Quantum Probabilities
What to Make of Aspect’s and Subsequent Empiricism
Examining and Reassessing Aspect’s Empirical Results
Exposition by Simulation
Concluding Comments
Full Text
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