SECTION 12 — THE ICOSAHEDRAL SUBSTRATE AND GAUGE INVARIANTS (v11.3)
By John Gavel
12.0 Overview
In Temporal Flow Physics (TFP), the Standard Model coupling values, weak mixing angle, and W/Z mass scales are not fundamental primitives. Instead, they emerge as topological and phase-volume invariants of a discrete substrate:
- K = 12 adjacency shell
- H = 132 handshake budget per site
- Icosahedral packing and routing constraints
- Holonomy around causal loops
- Phase coherence of multi-path motifs
This section derives these quantities from first principles, linking observables to substrate geometry and combinatorial capacity established in Sections 2–11.
12.1 Icosahedral Phase Volume (Omega) — the lepton linear coefficient
Define substrate parameters:
- K = 12
- eta_sub = H / K² = 132 / 144 = 11/12
- Φ = Golden Ratio = (1+√5)/2
- Ξ = Φ² / √3
The Icosahedral Phase Volume captures radial handshake capacity per axis:
Ω = (π √(K − 1)) / (Ξ · η_sub) ≈ 7.517
Impact on lepton masses:
- Spinor-locking projection = (1 − 1.5 / K)
- Linear coefficient in lepton mass law: C_L = Ω · (1 − 1.5 / K) ≈ 6.585
Interpretation: The linear term in lepton masses is a first-principles phase-volume projection of the K = 12 lattice, reduced by spinor constraints.
12.2 Fine-structure constant α as substrate impedance
α arises as the relational cost of routing a unit alignment change in the 132-bit substrate. Ingredients:
- H = 132 (core handshake addresses)
- δ_conflict = 3 (three independent failure channels — branching, phase, temporal — each contributing ~1 bit of unresolved tension at the vertex level)
- Ψ_sph ≈ 0.9396926208 (fractional handshake loss projecting ideal sphere onto 12-vertex icosahedral lattice)
- Gauge-holonomy contribution = 2π
- Φ = Golden Ratio
- Φ⁻² = discrete curvature correction
Exact first-principles formula:
α⁻¹ = H(K−1)/(K Ψ_sph) + 2π + Φ + Φ⁻²
Stepwise numeric evaluation:
- H(K−1)/(K Ψ_sph) = 132 × 11 / (12 × 0.9396926208) ≈ 128.753
- 2π + Φ + Φ⁻² ≈ 6.2831853072 + 1.6180339887 + 0.3819660113 ≈ 8.2831853072
- Total α⁻¹ ≈ 128.753 + 8.283185 ≈ 137.036185
Experimental α⁻¹ = 137.035999084. Agreement within 0.00014%. Interpretation: The fine-structure constant is the **substrate impedance to unit chiral flow**, emerging purely from discrete coordination, icosahedral geometry, golden-ratio symmetry, and holonomy constraints — no free parameters are introduced.
12.3 Gauge bosons as lattice resonances (edge vs. vertex modes)
Gauge excitations are collective phase updates of the lattice:
- W boson: edge resonance along adjacency backbone
- Z boson: vertex/face resonance, volumetric closure cost
Working formulas:
M_W ≈ M_p √H (Ω / Lag)
M_Z ≈ M_W · (R_vertex / ρ_edge) ≈ M_W · 1.1342
Definitions:
- Lag ≡ <τ_routed> / τ₀ — average substrate ticks to propagate a handshake along an adjacency edge under finite K=12 routing and local tension, capturing propagation overhead / phase compression
- R_vertex / ρ_edge ≈ 1.1342 — vertex-to-edge geometric factor (icosahedral midradius / circumradius ratio)
Interpretation: W and Z masses are **geometric standards of the lattice**, with other boson and lepton scales shadowing these via phase-volume projections.
12.4 Weinberg angle from Golden mixing
Weak mixing angle is axial projection of orthogonal golden rectangles in the icosahedral skeleton:
sin²θ_W = 1 / Φ³ ≈ 0.236
Interpretation: Measures axial transfer between 12-vertex fermionic routing and 30-edge bosonic propagation channels. Substrate corrections reduce this to the physical value ≈ 0.231.
12.5 Cluster phase coherence and gauge stiffness
Define cluster order parameter:
Z_cluster = ∑_{i ∈ M} exp(i · θ_i)
C_θ = |Z_cluster| / |M| ∈ [0,1]
Phase stiffness (resonance impedance) ρ_s is a function of substrate geometry and handshake congestion. Relations:
- C_L ≈ Ω · (1 − DOF_eff / K), with DOF_eff ≈ 1.5 (half-spin degrees)
- α_EM ∝ 1 / C_θ²
- Volumetric saturation (Γ ≈ 1.273) rescales coherent limit to observed α⁻¹ ≈ 137
12.6 Neutrino mass from double-cycle parity residue
M_ν ≈ M_e · (1/H)² · (1 / (2H)) ≈ M_e / 264 ≈ 0.11 eV Neutrinos are parity-residue excitations (720° spinor update), suppressed by finite handshake ledger bookkeeping.
12.7 Strong-force stiffness and pentagonal angular deficit
Strong-force exponent: Z_strong scaling = 5 / 4 = 1.25 Origin: Closing a 3D vertex with 5-fold (pentagonal) symmetry. Angular deficit relative to flat 6-fold tiling produces topological impedance → strong stiffness and confinement.
12.8 Quark mixing (CKM) from face-area flux and hardware correction
Cabibbo angle (hardware-corrected):
θ_12 ≈ arcsin(1 / Φ³) · [H − (K / Φ)] / H ≈ 13°
Φ = Golden Ratio, H = 132, K = 12 Interpretation: Corrects ideal combinatorial angle for finite handshake tension. Higher CKM angles derived via octahedral/tetrahedral substructures.
12.9 Axiomatic closure (constants from substrate drivers)
| Observable | Substrate Origin | TFP Axioms |
|---|---|---|
| α⁻¹ | H, folding tax Ψ_sph, holonomy | A2, A3, A6 |
| M_W | edge-adjacency resonance, Lag | A2, A3, A6 |
| M_Z / M_W | vertex-to-edge ratio ≈ 1.1342 | A2, A3 |
| sin²θ_W | 1 / Φ³ | A3 |
| Z_strong exponent | pentagonal angular deficit 5/4 | A2, A3, A6 |
12.10 Saturation limit and the top quark
Top quark = endpoint of hadronic holonomy capacity: D = 32 recursion depth consumes budget: 122 bits lag + 10 bits update ≈ 132 bits Beyond this, motifs decay rather than hadronize → top mass signals lattice budget saturation Higgs mass: equilibrium junction excitation consistent with saturation picture
12.11 Interpretation and continuity
All electroweak and strong parameters emerge from the finite 132-bit substrate, realized by:
- Icosahedral packing logic
- Phase-volume constraints
- Loop holonomy and routing latency
No new fundamental couplings are introduced. α, weak mixing, W/Z mass scales, and strong-stiffness exponents are consequences of:
- Topology (icosahedral projection)
- Handshake budget arithmetic (H = 132, H_total = 140)
- Phase-holonomy closure conditions
Bridge to Section 13: Multi-path causal multiplets and holonomy produce SU(N) structure and fermionic multiplets consistent with the invariants above.
No comments:
Post a Comment