Lattice QCD Dominates Search; No Burnside Hexagonal Orbit Enumeration Found — E8 Intelligence Research

FINDING: The search results are dominated by lattice QCD papers, not Burnside's lemma or crystallographic point group orbit enumeration. The only direct hit on hexagonal lattice structure is a graphene simulation paper, but it uses a square lattice formulation, not hexagonal. No Burnside's lemma application to hexagonal crystallographic orbits is present in the returned set. | MATH: No explicit Burnside enumeration equations appear. The graphene paper references the massless Dirac equation: \( iγ^μ ∂_μ ψ = 0 \) in 2+1D, with Fermi velocity \( v_F ≈ 10^6 \, m/s \) replacing \( c \). Lattice QCD papers use the QCD action: \( S = ∫ d^4x \, ψ̄(iγ^μ D_μ - m)ψ - 1/4Fμν^a Faμν \), with lattice spacing \( a \) and quark masses \( m_q \). No golden ratio, 0.382, 0.618, 0.786, 1.618, or 2.618 constants appear anywhere. | CONNECTION: The hexagonal lattice of graphene has \( D₆ₕ \) point group symmetry (order 24), whic Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com