Void-Pair Conservation as the Physical Mechanism of Quantum Entanglement and Bell Correlations

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1. Verfasser: Martin, Luke
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author Martin, Luke
author_facet Martin, Luke
contents <p>We propose that quantum entanglement is the physical manifestation of void-pair conservation in a quantized vacuum foam. The conservation law B(x) + V(x') = D requires that every vacuum displacement event D creates exactly one bubble B at position x and one complementary void V at position x'. Entangled particles are two addresses of one displacement event — not two correlated objects but two endpoints of one physical thing. This escapes Bell's theorem without local hidden variables: Bell's factorization assumption requires the correlation function to be writable as a product of local functions, but D is inherently non-local and cannot be so factored. The antipodal symmetry of the void-pair uniquely selects the quantum singlet state, producing the experimentally confirmed correlation E(a,b) = -cos(theta_ab). We verify numerically that the model reproduces the full quantum mechanical CHSH violation S = 2*sqrt(2). We propose a testable prediction for three-particle connected foam topologies that differs from the standard GHZ prediction.<br><br>UFFT Paper #2. Part of the Unified Foam Field Theory (B + V = D). Zero free parameters.<br>GitHub: <a class="underline underline underline-offset-2 decoration-1 decoration-current/40 hover:decoration-current focus:decoration-current" href="https://github.com/WebEnvy/UnifiedFoamFieldTheory">https://github.com/WebEnvy/UnifiedFoamFieldTheory</a></p>
format Recurso digital
id zenodo_https___doi_org_10_5281_zenodo_18706806
institution Zenodo
language
publishDate 2026
publisher Zenodo
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spellingShingle Void-Pair Conservation as the Physical Mechanism of Quantum Entanglement and Bell Correlations
Martin, Luke
quantum entanglement
Bell's theorem
hidden variables
vacuum structure
non-locality
quantum foundations
void-pair conservation
singlet state
UFFT
truncated octahedron
face Laplacian
foam lattice
<p>We propose that quantum entanglement is the physical manifestation of void-pair conservation in a quantized vacuum foam. The conservation law B(x) + V(x') = D requires that every vacuum displacement event D creates exactly one bubble B at position x and one complementary void V at position x'. Entangled particles are two addresses of one displacement event — not two correlated objects but two endpoints of one physical thing. This escapes Bell's theorem without local hidden variables: Bell's factorization assumption requires the correlation function to be writable as a product of local functions, but D is inherently non-local and cannot be so factored. The antipodal symmetry of the void-pair uniquely selects the quantum singlet state, producing the experimentally confirmed correlation E(a,b) = -cos(theta_ab). We verify numerically that the model reproduces the full quantum mechanical CHSH violation S = 2*sqrt(2). We propose a testable prediction for three-particle connected foam topologies that differs from the standard GHZ prediction.<br><br>UFFT Paper #2. Part of the Unified Foam Field Theory (B + V = D). Zero free parameters.<br>GitHub: <a class="underline underline underline-offset-2 decoration-1 decoration-current/40 hover:decoration-current focus:decoration-current" href="https://github.com/WebEnvy/UnifiedFoamFieldTheory">https://github.com/WebEnvy/UnifiedFoamFieldTheory</a></p>
title Void-Pair Conservation as the Physical Mechanism of Quantum Entanglement and Bell Correlations
topic quantum entanglement
Bell's theorem
hidden variables
vacuum structure
non-locality
quantum foundations
void-pair conservation
singlet state
UFFT
truncated octahedron
face Laplacian
foam lattice
url https://doi.org/10.5281/zenodo.18706806