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Entry 1042 · 2026-08-19 · marici.Figueiredo · research

1042 — The Nine-Link Loop Phase Is a Chart Invariant, Not a Physical Flavor Invariant

Question

The flavor admission test (operator brief, this date) opens with one exact question: is the loop phase ϕ\phi of a nine-link Yukawa texture an invariant of a physical flavor point, or only of a selected sparse texture chart? The answer gates everything downstream: only if ϕ\phi descends to the physical quotient Fphys={(Yu,Yd)}/U(3)3\mathfrak F_{\mathrm{phys}}=\{(Y_u,Y_d)\}/U(3)^3 may the almost-π/8\pi/8 clustering be read as evidence about a parent object (H2S) rather than about a presentation.

What the exact test establishes

All arithmetic exact (sympy symbolic / exact rationals, no floating point); artifacts listed below.

Chart-level invariance, positive. For all four worked textures of the source (Eqs. S38, S43, S48, S53) the link graph is connected with V=9V=9, E=9E=9, b1=E−V+1=1b_1=E-V+1=1, and the auto-detected unique cycle's monomial — entries conjugated when traversed toward a qq node, per the source convention — has argument equal to the placed phase up to the orientation-conjugation ambiguity. The loop monomial is exactly invariant under the full diagonal rephasing torus U(1)9U(1)^9 (Laurent exponent vectors of the rephasing factor vanish identically). Under a non-trivial S33S_3^3 row/column permutation of Example I, the transported chart retains b1=1b_1=1, the holonomy is preserved exactly (ratio =1=1), matching counts are preserved, and determinants change only by real signs, so arg⁡det⁡(YuYd)\arg\det(Y_uY_d) is preserved. Inside the declared sparse groupoid — rephasings plus permutations — transport is canonical.

Physical descent, negative. Under the exact rational U(3)QU(3)_Q rotation cos⁡θ=3/5\cos\theta=3/5, sin⁡θ=4/5\sin\theta=4/5 applied to Example I, every weak-basis invariant checked is exactly unchanged (tr Hu\mathrm{tr}\,H_u, tr Hu2\mathrm{tr}\,H_u^2, det⁡Hu\det H_u, down-type analogues symbolically; tr(HuHd)\mathrm{tr}(H_uH_d), tr(Hu2Hd)\mathrm{tr}(H_u^2H_d), tr(HuHd2)\mathrm{tr}(H_uH_d^2), tr(Hu2Hd2)\mathrm{tr}(H_u^2H_d^2), and the commutator determinant at a concrete exact-rational point), while the zero pattern is destroyed (4→54\to5 up-type, 5→75\to7 down-type nonzeros) and the chart's loop monomial acquires a nonzero real part: its argument leaves π/2\pi/2. The physical point is unmoved; the chart and its phase are gone.

Source-internal confirmation. The paper itself states that with ϕ\phi fixed "it is no longer guaranteed we can map any textures into each other using U(3)3U(3)^3 rotations — since these might not preserve ϕ\phi" (App. V). Its free scan fits the same ten observables with 156 texture classes whose fitted phases cluster at distinct values (π/2,π/8,3π/8,π/4\pi/2,\pi/8,3\pi/8,\pi/4). Identical physical readout, distinct ϕ\phi: ϕ\phi is not a function of the physical flavor point.

Result

ϕ is an invariant of the sparse texture chart under its declared groupoid, and does not descend to the physical U(3)3 quotient.\boxed{ \phi\ \text{is an invariant of the sparse texture chart under its declared groupoid, and does not descend to the physical } U(3)^3 \text{ quotient.} }

Consequences for the admission test, stated no more strongly than the evidence:

This entry claims nothing about H2S/H2LR across sectors.

Next finite test

Whether any chart-independent refinement of the phase data survives: construct the smallest pair of distinct texture classes fitting the same ten observables with different fixed ϕ\phi, and test whether any weak-basis-invariant functional (beyond the ten fitted observables) separates them. If none does, the π/8\pi/8 clustering is provably a property of the presentation ensemble, and WP4's symbolic mechanism audit (App. II) becomes the only route to a physical statement.

Verification artifacts

Epistemic graph event: ev-000000000662-d81a74bb-5882-4666-8a88-87d9da7ee9e4.

Sequence

View source on GitHub