Theoretical analysis demonstrates a geometric coordinate mapping for tetrahedral Bell correlations in four-dimensional space, revealing a null physical residual beyond standard quantum boundaries.
Version 0.4 carries the previously open tetrahedral/Bell branch through an explicit mathematical formalisation. It separates a four-context indexing simplex and Boolean restriction lattice from the Bell-native tetrahedral CHSH facets in R^4, formalises sign-to-context semantic attachment, and derives the exact Facet-adapted Tetrahedral Bell Chart E = Vλ + (ν/4)c with 1ᵀλ = 1. The three independent λ coordinates carry the selected facet address and ν = S_c(E) − 2 supplies the fourth transverse correlator coordinate, resolving the prior four-versus-three degree-of-freedom objection without forcing a tetrahedron to encode unrestricted four-correlator data by itself. The paper further treats marginal-fibre reopening, exact one-correlator ablation/restoration, the local/Tsirelson/PR normal-ray benchmarks, and a natural four-volume candidate that collapses exactly to |S−2|/3. After subtraction of native Bell/Fine/Tsirelson-Landau-Masanes ownership and a reparameterisation test, no independent new Bell inequality, quantum boundary, or physical mechanism survives; the current physical residual is null.
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Mark Charles McLaughlin (2026) studied this question.
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