Randomized trial establishes placement theorems for Higgs and fermion chirality, implying unique outcomes supported by geometry.
We prove that the Standard Model particle content is not merely consistent with the geometry of the truncated octahedron (Kelvin cell): it is the only possible outcome. Two placement theorems are established. The framework uses two distinct torsion operators, named explicitly in this version: the scalar torsion charge is the eigenvalue under T_hex = (1/3)·A_hh, the degree-normalised adjacency of the hexagonal subgraph (the cube graph); the chiral structure lives in the inter-type operator T = P_sq·L·P_hex − P_hex·L·P_sq. Theorem 57.1 (Higgs Necessity): of the two scalar (spin-0) irreps of O_h, namely A₁g and A₂u, only A₂u can drive spontaneous symmetry breaking. Under T_hex, A₁g carries charge +1 (positive effective mass², stable vacuum) and A₂u carries charge −1 (the bipartite minimum of the cube graph: negative effective mass², origin unstable). SSB is forced for A₂u and forbidden for A₁g. The Higgs is A₂u by exhaustion of alternatives. Theorem 57.2 (Chiral Structure): from T²|T₁u = −4·I (Theorem 56.1), the inter-type operator T has purely imaginary eigenvalues ±2i on the T₁u subspace, and T is purely cross-block between the two T₁u bands: chirality eigenstates are equal-weight superpositions of the r₁ and r₂ bands, exactly as γ⁵ eigenstates superpose mass eigenstates in Dirac theory. The labelling T₁u(r₁) = left-handed, T₁u(r₂) = right-handed is fixed by the B+V=D orientation of T together with the Eg-coupling argument (T₁u(r₁) carries square-face content (1+1/√17)/2 ≈ 62%, hence the stronger coupling to the pure-square electroweak Eg sector). The chiral structure is a theorem; the band labelling is a derived identification conditional on that coupling argument.Changes in version 2.0: the two torsion operators conflated in v1.0 are now named and separated (T_hex scalar charges vs the inter-type operator T); the premises of Theorem 57.1 are corrected (conclusion unchanged); the v1.0 claim that the +2i eigenvectors localise in the T₁u(r₁) band is withdrawn (they are exactly 50/50 across the two bands, and the band labelling is now a stated conditional identification); the Section 2 dimension table and Section 6 Weinberg angle line are corrected. All corrections are machine-verified in verify_FtF_audit_2026-07.py in the repository.
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Luke Martin (2026) studied this question.
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