Part VI — Phenomenology

Masses, Couplings, and Falsifiable Patterns
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Abstract

Part VI confronts the Dual–Flux (DF) framework with particle-level phenomenology using only the structural ingredients fixed in Parts I–V. No new dynamical kernels or independent mass scales are introduced. All empirical inputs are limited to measured quantities—the charged-lepton masses, sin2θW(mZ), GF, and a single dimensionless hadronic slope ratio—while all additional coefficients remain O(1) projector weights fixed by DF sector geometry. Every observable discussed here follows from the present-surface geometry, the TDGL memory kernel, and the sector projectors acting on closed states.

We show first that the three gauge couplings at the electroweak scale {α, α2, α3} emerge from a single present-only scale α*, determined by the DF–Foot lepton analysis, together with the short/long memory ratio w(μ) extracted from the weak mixing angle. A small, non-resonant 2π contribution of the long-memory kernel then reproduces the observed electromagnetic running from mZ down to zero momentum. The same stiffness scale, combined with GF, fixes mW and mZ at tree level, while the Higgs mass appears as a curvature eigenvalue of the scalar projector, requiring no new dimensionful input.

Mixing matrices arise from small inter-sector leakage on the present surface. The contrast between small CKM and large PMNS angles follows from the DF mass = memory hierarchy and neutrino quasi-degeneracy, while CP violation results from the product of torsion and leakage. This yields sharp no-go signatures: inverted CKM/PMNS hierarchies or vanishing lepton-sector CP phases would falsify DF at the interaction level.

Lifetimes and decay widths follow from the imaginary part of the TDGL kernel after present-closure. Unstable states correspond to differentiated coherons whose loops cannot be sustained by finite present-memory, providing a unified account of the observed hierarchy from stable neutrinos and electrons to rapidly decaying heavy quarks and broad W, Z resonances. Photon interference in double-slit setups is similarly described as linear propagation of non-anchored Φ+ flux on Σpresent, with the disappearance of fringes at large distances controlled solely by the finite depth of the present-memory functional, without any collapse postulate.

Overall, Part VI shows that DF can reproduce a broad set of couplings, mass relations, mixing patterns, lifetimes, and interference phenomena using only present-surface geometry, the TDGL memory kernel, and a small set of dimensionless anchors. This places the theory at a point where cosmological tests become the next natural and unavoidable step.

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