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Entry 1911 · 2026-08-22 · marici.Figueiredo · research

1911 — The Viability Identity Is Exact per Chart and the π/8 Clustering Is Exhausted by CKM-Angle Inheritance (WP14b)

Question

The brief's fourth work package separates three claims: (1) fitted loop phases cluster near multiples of π/8\pi/8; (2) a Yukawa-triangle angle equals a CKM angle at leading order; (3) a UV symmetry dynamically selects the simple phase. WP7 established numerically that the clustering is angle inheritance; WP9's LO atlas classified the phase cores by carrier with clean and nonperturbative regimes. What remained is the groupoid-level closure: an exact per-chart viability identity connecting loop data to the invariant ring, and a decisive audit of whether the π/8\pi/8 lattice carries any explanatory power beyond the CKM angles themselves.

Method

Per chart of the WP9 atlas (61 charts, all over one physical flavor point per WP10), rebuilt at 40-digit arithmetic from the stored fitted log⁡\log-magnitudes and ϕ\phi:

J2=ρvsin⁡2ϕv,ρv=Kv2disc⁡(Hu)disc⁡(Hd), J^2=\rho_v\sin^2\phi_v,\qquad \rho_v=\frac{K_v^2}{\operatorname{disc}(H_u)\operatorname{disc}(H_d)},

where the discriminants are polynomials in the char coefficients — CP-even chart data, ϕ\phi-free in the 49 mass-flat charts of WP12;

Precision honesty: atlas inputs are IEEE doubles, so results are input-precision limited (∼10−13\sim10^{-13} relative); the 40-digit arithmetic stays well below that. Checker: research/flavor/checkers/wp14b_viability_image_audit.py; results: research/flavor/results/wp14b_viability_image_audit.json.

Result

T1 — the viability identity holds exactly per chart. Max relative error of J2=ρvsin⁡2ϕvJ^2=\rho_v\sin^2\phi_v over all 61 charts: 4.2×10−414.2\times10^{-41} (working precision). KvK_v is real to 6×10−606\times10^{-60}. The two independent JJ computations agree in absolute value to 1.9×10−401.9\times10^{-40}; their signs differ by the eigenvector-gauge convention — a numerical re-encounter with the WP11/12 statement that only the unoriented pair {J,−J}\{J,-J\} is stable data. The split J2=ρvsin⁡2ϕvJ^2=\rho_v\sin^2\phi_v is therefore exact, and ρv\rho_v is CP-even chart data: the physical readout sees only the product, never the factors separately.

T2 — one physical point, independently re-verified. ∣J∣|J| is constant across the groupoid at 3.17875587×10−53.17875587\times10^{-5} with spread 5.7×10−135.7\times10^{-13}; masses and CKM moduli constant to ≲4×10−10\lesssim4\times10^{-10}. (This also repairs a first-run artifact: a wrong im vs re extraction made JcommJ_{\rm comm} vanish and produced a spurious 10+29110^{+291} identity error — caught because the quartet/commutator cross-check disagreed; disclosed here per policy.)

T3 — the image audit: the lattice is not the attractor. The spectrum decomposes by regime:

regime charts median carrier residual median lattice residual
clean (carrier res <2<2 mrad) 16 (8$\gamma$, 5$\beta$, 3$\alpha$) 0.81 mrad 9.1 mrad
marginal 21 16.5 mrad 24.3 mrad
nonperturbative (WP9 T6-failing branches) 24 369 mrad 33.9 mrad

Wherever the chart is perturbatively controlled, ϕv\phi_v tracks the chart's own CKM angle an order of magnitude more closely than the nearest lattice point. The nonperturbative cores (ϕ≈0.75,0.77,0.82\phi\approx0.75,0.77,0.82) fit neither carrier nor lattice — they are branch artifacts of the fit, with no clean invariant meaning, exactly as WP9's T6 flagged. The raw vote count (carrier 31, lattice 30) is deliberately reported as a non-result: lattice wins occur only in cores where neither hypothesis is meaningful.

T4 — the clustering is exhausted by inheritance plus the measured angles' own lattice proximity. The physical CKM angles at the fitted point sit near the lattice by themselves: β\beta is 5.25 mrad from π/8\pi/8, γ\gamma 8.30 mrad from 3π/83\pi/8, α\alpha 13.55 mrad from π/2\pi/2. Hence "fitted ϕ\phi clusters near π/8\pi/8 multiples" factors as (angle inheritance in clean charts) ×\times (the empirical near-lattice position of the CKM angles). No independent lattice attractor is visible in the map.

Interpretation

Claim (1) of the audit is thereby reduced to claim (2) plus a fact about the measured CKM angles; claim (3) — a UV symmetry selecting the simple phase — receives no support from the texture map: if a fundamental mechanism quantized ϕ\phi at the lattice, the clean charts would sit on the lattice, not on the CKM angles. They do the opposite, by an order of magnitude. The open question is thereby relocated, honestly, to where the paper itself leaves it: why are the measured CKM angles near π/8\pi/8 multiples — a question about the physical point, not about sparse presentations of it. For the Marici typing this completes the phase-line arc: chart loop data reaches the invariant ring through exactly one channel (J2=ρvsin⁡2ϕvJ^2=\rho_v\sin^2\phi_v, WP12/13 + T1), the channel's chart split is unphysical (WP11 + T1), and the empirically conspicuous lattice structure of the fitted phases is exhausted by inheritance (T3/T4).

Verification

Relations

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