Local hidden variable modelling, classicality, quantum separability, and the original Bell inequality
Elena R. Loubenets

TL;DR
This paper establishes a general, experimentally verifiable condition for the validity of Bell's original inequality within local hidden variable models, highlighting differences between classicality and quantum separability.
Contribution
It introduces a broad class of quantum states that satisfy Bell's original inequality without requiring perfect correlations, expanding understanding of quantum separability and classicality.
Findings
Identifies a general condition for Bell inequality validity in LHV models.
Shows that certain quantum states satisfy Bell's original inequality without perfect correlations.
Highlights the distinction between classicality and quantum separability beyond CHSH inequality.
Abstract
We introduce a general condition sufficient for the validity of the original Bell inequality (1964) in a local hidden variable (LHV) frame. This condition can be checked experimentally and incorporates only as a particular case the assumption on perfect correlations or anticorrelations usually argued for this inequality in the literature. Specifying this general condition for a quantum bipartite case, we introduce the whole class of bipartite quantum states, separable and nonseparable, that (i) admit an LHV description under any bipartite measurements with two settings per site; (ii) do not necessarily exhibit perfect correlations and may even have a negative correlation function if the same quantum observable is measured at both sites but (iii) satisfy the "perfect correlation" version of the original Bell inequality for any three bounded quantum observables A, A'=B, B' at sites "A"…
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