We propose and develop the central mechanism behind all coupling constant scaling in the brane-bulk octonionic framework: at energy E, a focal zone cannot be localised to a single Fano lattice node but occupies a quantum superposition of neighbouring nodes, with overlap probability Pij (E) ∝ (E/mPl) ∆ij where ∆ij is the topological distance between nodes i and j on the Fano graph. At the Planck scale, all seven nodes are in complete superposition no focal zone can be resolved as belonging to a single node and all coupling constants converge to a common G2-symmetric value: gauge unication is the complete delocalization of the Fano eigenmodes. As energy decreases from mPl, the eigenmodes localise back onto their characteristic nodes at a rate governed by the Fano Laplacian eigenvalue λi ∈0, 4, 7: higher-λ modes localise faster, giving steeper running. The three gauge coupling constants correspond to the three Fano eigenmode families: αs ↔λ = 7 (fastest localisation, steepest running, asymptotic freedom) ; αW ↔λ = 4 (intermediate) ; αem ↔ λ = 0 (softest mode, slowest running). Asymptotic freedom in QCD emerges because at high energy the H+/H−sector distinction blurs through node superposition, reducing the cross-sector bridge formation amplitude of Paper LVIII and hence αs. The one-loop beta function coecients are identied with the Fano Laplacian eigenvalues weighted by the Fano mode census; the exact coecients require the census computation deferred from Paper LIII, but the ratios of running rates are xed by λ = 7: 4: 0 from the lattice geometry alone. Five new predictions follow (Predictions 110114). Part of the One-Octonion Brane-Bulk Framework series. Anchor DOI: 10. 5281/zenodo. 19120873. Community: one-octonion-brane-bulk. Author: Bharathi Dasan Jagadeesan, M. D. , University of Minnesota. ORCID: 0000-0002-1143-941X.
Bharathi Jagadeesan (2026) studied this question.