Quantum Violations of CHSH-3 Inequality via Tensor Product Hilbert Spaces — E8 Intelligence Research

FINDING: The CHSH-3 inequality extends the standard CHSH framework to three measurement settings per party, with quantum violations computable via semidefinite programming; the Hilbert space structure underpinning these violations is the tensor product of local Hilbert spaces, with singular values of the correlation matrix determining maximal violation bounds. | MATH: Standard CHSH: \(S = \langle AB \rangle + \langle AB' \rangle + \langle A'B \rangle - \langle A'B' \rangle \leq 2\) (local), \(S_{\text{quantum}} \leq 2\sqrt{2} \approx 2.828\). CHSH-3 generalizes to three settings per party, with the quantum bound given by the maximal singular value of the correlation tensor \(T_{ij} = \langle A_i \otimes B_j \rangle\), i.e., \(\|T\|_\infty \leq \sqrt{3}\) for the specific CHSH-3 form (Tsirelson-type bound). The Hilbert space is \(\mathcal{H}_A \otimes \mathcal{H}_B\), and the singular value decomposition of the \(3 \times 3\) correlation matrix yields singular values \(\sigma_1 \geq \si 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
2026-10-17
DOI
https://doi.org/10.5281/zenodo.23431332
Primary Topic
Quantum Mechanics and Applications
Type
preprint
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preprint

Quantum Violations of CHSH-3 Inequality via Tensor Product Hilbert Spaces — E8 Intelligence Research

Andrew Stewart Caldin
Zenodo (CERN European Organization for Nuclear Research)
Quantum Mechanics and Applications
preprint

Quantum Violations of CHSH-3 Inequality via Tensor Product Hilbert Spaces — E8 Intelligence Research

Andrew Stewart Caldin
preprint en

Abstract

FINDING: The CHSH-3 inequality extends the standard CHSH framework to three measurement settings per party, with quantum violations computable via semidefinite programming; the Hilbert space structure underpinning these violations is the tensor product of local Hilbert spaces, with singular values of the correlation matrix determining maximal violation bounds. | MATH: Standard CHSH: \(S = \langle AB \rangle + \langle AB' \rangle + \langle A'B \rangle - \langle A'B' \rangle \leq 2\) (local), \(S_{\text{quantum}} \leq 2\sqrt{2} \approx 2.828\). CHSH-3 generalizes to three settings per party, with the quantum bound given by the maximal singular value of the correlation tensor \(T_{ij} = \langle A_i \otimes B_j \rangle\), i.e., \(\|T\|_\infty \leq \sqrt{3}\) for the specific CHSH-3 form (Tsirelson-type bound). The Hilbert space is \(\mathcal{H}_A \otimes \mathcal{H}_B\), and the singular value decomposition of the \(3 \times 3\) correlation matrix yields singular values \(\sigma_1 \geq \si 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 Mechanics and Applications
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