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Theoretical derivation demonstrates the emergence of Dirac spinors and Standard Model symmetries from correlation operator algebras, indicating a pre-geometric origin of matter and gauge interactions.
We derive 3+1D Dirac spinors and the Standard Model gauge algebra su(3) ⊕ su(2) ⊕ u(1) directly from the non-local operator algebra A_I defined on the admissible correlation manifold B_adm. Parity-odd antisymmetric correlation fluctuations δI_- generate a canonical Clifford algebra {γ^μ, γ^ν} = 2gμν[I], producing emergent Grassmannian Dirac fields ψ(x). The maximal continuous automorphism group of the local correlation fiber F_x factorizes uniquely into SU(3) × SU(2) × U(1), yielding the full Standard Model gauge structure without postulates. Evaluating the effective average action Γ_k[I] at the functional renormalization group fixed point α* ≈ 0.139 produces the minimal gauge-covariant derivative D_μ = ∂_μ − ig_3 G_μ^a T^a − ig_2 W_μ^i τ^i − ig_1 Y B_μ and the complete Dirac–Yang–Mills Lagrangian unified with gravity. Matter fields, gauge interactions, and spacetime geometry emerge as forced geometric deformations of the pre-geometric correlation substrate I(x,x'), establishing Theorem III.3 and completing the matter–gauge emergence layer of UN Theory.
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Clint Jefferys (2026) studied this question.
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