Derives gauge algebra components from correlation operator algebras, suggesting a new structure in field theory.
This paper derives 3+1D Dirac spinors and the Standard Model gauge algebra su(3) ⊕ su(2) ⊕ u(1) directly from the non-local correlation operator algebra A_I defined on the correlation manifold B_adm. It proves that parity-odd, anti-symmetric bi-local correlation modes δ I_- generate a canonical Clifford algebra {γ^μ, γ^ν} = 2 g^μ^ν[I] I4, producing 4-component Grassmannian Dirac spinor fields ψ(x) and ψ̄(x) without assuming primitive spinor structures. Furthermore, by examining the local correlation fiber F_x ⊂ T_xM ⊕ (T_xM ⊗ T_xM), the maximal continuous Lie algebra of fiber automorphisms preserving positivity, complex structure, and trace-class normalization is shown to factorize uniquely into su(3) ⊕ su(2) ⊕ u(1). Evaluating the effective average action C_k[I] at the FRG fixed point alpha = 0.139 forces the gauge-covariant derivative Dμ and yields the complete, gauge-invariant Dirac-Yang-Mills action.
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Clint Jefferys (2026) studied this question.
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