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This paper offers a pedagogical visualization of Bell inequalities using an analogy between entangled particles and "twins" answering questions about daily meals, clarifying the geometric relationship between local models, quantum states, and no-signalling regions. While the breakfast/lunch/dinner metaphor serves as an accessible entry point, the core contribution remains firmly within fundamental quantum information theory rather than applied AI or machine learning.
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From breakfast, lunch, and dinner to the Bell-inequality tetrahedron

arXiv2 min read

arXiv:2609.14436v1 Announce Type: new Abstract: A simple pedagogical discussion and visualization of certain Bell inequalities is presented with the help of a system involving two \textquotedblleft twins\textquotedblright, originally discussed in 2605.03104. These twins answer identically when the same `question' is posed, here exemplified with: Did you like breakfast/lunch/dinner? In analogy, for two entangled particles at distant locations, the `twin-like' quantum state is such that the same outcome for the same measurement (i.e. spin direction) is obtained. In the space $(X,Y,Z)$ of mixed moments (i.e. $X$ refers to breakfast-lunch correlation, being $1$ for same answers and $-1$ for opposite ones), the space of Bell local models is contained in a tetrahedron, while the quantum space is bound by an elliptope that embeds the tetrahedron. The whole no-signalling region in the $(X,Y,Z)$ space is the cube $[-1,1]^{3}.$ The twin scenario applies e.g. to the decay of the Higgs into fermions.

Abstract:A simple pedagogical discussion and visualization of certain Bell inequalities is presented with the help of a system involving two \textquotedblleft twins\textquotedblright, originally discussed in 2605.03104. These twins answer identically when the same `question' is posed, here exemplified with: Did you like breakfast/lunch/dinner? In analogy, for two entangled particles at distant locations, the `twin-like' quantum state is such that the same outcome for the same measurement (i.e. spin direction) is obtained. In the space $(X,Y,Z)$ of mixed moments (i.e. $X$ refers to breakfast-lunch correlation, being $1$ for same answers and $-1$ for opposite ones), the space of Bell local models is contained in a tetrahedron, while the quantum space is bound by an elliptope that embeds the tetrahedron. The whole no-signalling region in the $(X,Y,Z)$ space is the cube $[-1,1]^{3}.$ The twin scenario applies e.g. to the decay of the Higgs into fermions.

8 pages, 3 figures. Prepared for the proceedings of the Workshop on Quantum Entanglement, 3-4 July 2026, Jagiellonian University, Krakow, Poland. this https URL

arXiv:2609.14436 [quant-ph]

(or arXiv:2609.14436v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2609.14436 arXiv-issued DOI via DataCite (pending registration)

Full text under the publisher's open licence · 182 words

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