Abstract

We start with a review on classical probability representations of quantum states and observables. We show that the correlations of the observables involved in the Bohm–Bell type experiments can be expressed as correlations of classical random variables. The main part of the paper is devoted to the conditional probability model with conditioning on the selection of the pairs of experimental settings. From the viewpoint of quantum foundations, this is a local contextual hidden-variables model. Following the recent works of Dzhafarov and collaborators, we apply our conditional probability approach to characterize (no-)signaling. Consideration of the Bohm–Bell experimental scheme in the presence of signaling is important for applications outside quantum mechanics, e.g., in psychology and social science. The main message of this paper (rooted to Ballentine) is that quantum probabilities and more generally probabilities related to the Bohm–Bell type experiments (not only in physics, but also in psychology, sociology, game theory, economics, and finances) can be classically represented as conditional probabilities.

Highlights

  • This paper is directed to resolution of the old foundational problem of quantum mechanics: whether it is possible to represent quantum states by classical probability (CP) distributions and quantum observables by random variables [1]

  • The paper contains a brief review on CP-representations of the probabilistic structure of quantum mechanics

  • The main part of the paper is devoted to one special CP-representation based on the conditional probability interpretation of quantum probabilities

Read more

Summary

Introduction

This paper is directed to resolution of the old foundational problem of quantum mechanics: whether it is possible to represent quantum states by classical probability (CP) distributions and quantum observables by random variables [1]. We analyze the general measurement scheme involving compatible and incompatible observables which need not be described by the quantum formalism. Our starting point is construction of the CP-representation for quantum mechanics. Throughout the paper, we use capital Latin letters, A, B, R (with indexes) to denote observables and small letters a, b, r (with indexes) to denote classical random variables (RVs)

Towards CP-Representation
No-Go Statements
Conditional Probability Approach
CP-Representations in the Presence of Signaling
Bohm–Bell Type Experiment
Missed Component of Experimental Arrangement
Bohm–Bell Type Experiments
Complete CP-Model
Constraints on Joint Probabilities Implied by Matching Condition
Correspondence between Observational and Classical Conditional Probabilities
Violation of the CHSH-Inequality by Conditional Correlations
Construction of jpd from Observational Probabilities
No-Signaling in Quantum Physics
No-Signaling as a Condition of Independence of Random Variables
Interpretation of No-Signaling
Hidden-Variables Models
Findings
Conclusions
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call