Unifying Bell Inequalities and Entanglement Witnesses via Correlation Polytope Geometry — E8 Intelligence Research

FINDING: Buscemi's framework unifies Bell inequalities with entanglement witnesses via "semidefinite programming" and "facet structure" of correlation polytopes, showing quantum violations correspond to specific geometric facets. | MATH: Bell inequalities are linear inequalities over the correlation polytope \( \mathcal{P} \); quantum correlations form a convex set \( \mathcal{Q} \) strictly larger than \( \mathcal{P} \) (local hidden variable polytope). Buscemi's unification maps entanglement witnesses (Hermitian operators \( W \geq 0 \) with \( \mathrm{Tr}(W\rho) \geq 0 \) for separable \( \rho \)) to Bell-type inequalities via a "quantum channel" transformation. Key constants: the Tsirelson bound \( 2\sqrt{2} \) for CHSH, and the ratio \( 2\sqrt{2}/2 = \sqrt{2} \approx 1.414 \) (not a golden ratio, but a quadratic irrational). Facet structure: the polytope \( \mathcal{P} \) has facets defined by inequalities like \( \langle A_1B_1 \rangle + \langle A_1B_2 \rangle + \langle A_2B_1 \r Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

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Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-09-04
DOI
https://doi.org/10.5281/zenodo.22294680
Primary Topic
Quantum Information and Cryptography
Type
preprint
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Unifying Bell Inequalities and Entanglement Witnesses via Correlation Polytope Geometry — E8 Intelligence Research

Andrew Stewart Caldin
Zenodo (CERN European Organization for Nuclear Research)
Quantum Information and Cryptography
preprint

Unifying Bell Inequalities and Entanglement Witnesses via Correlation Polytope Geometry — E8 Intelligence Research

Andrew Stewart Caldin
preprint en

Abstract

FINDING: Buscemi's framework unifies Bell inequalities with entanglement witnesses via "semidefinite programming" and "facet structure" of correlation polytopes, showing quantum violations correspond to specific geometric facets. | MATH: Bell inequalities are linear inequalities over the correlation polytope \( \mathcal{P} \); quantum correlations form a convex set \( \mathcal{Q} \) strictly larger than \( \mathcal{P} \) (local hidden variable polytope). Buscemi's unification maps entanglement witnesses (Hermitian operators \( W \geq 0 \) with \( \mathrm{Tr}(W\rho) \geq 0 \) for separable \( \rho \)) to Bell-type inequalities via a "quantum channel" transformation. Key constants: the Tsirelson bound \( 2\sqrt{2} \) for CHSH, and the ratio \( 2\sqrt{2}/2 = \sqrt{2} \approx 1.414 \) (not a golden ratio, but a quadratic irrational). Facet structure: the polytope \( \mathcal{P} \) has facets defined by inequalities like \( \langle A_1B_1 \rangle + \langle A_1B_2 \rangle + \langle A_2B_1 \r Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

Zenodo (CERN European Organization for Nuclear Research)
Quantum Information and Cryptography
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