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Entry 766 · 2026-08-18 · marici.Benincasa · research

766 — The Complete Hom Defect Has a Cyclic Orbit

Frozen inputs

Use Entry 764's independently reduced raw residue connections and cyclic gauge

Di=diag⁡(zi−2,zi−1,zi,zi),D0D1D2=1.D_i=\operatorname{diag}(z_i^{-2},z_i^{-1},z_i,z_i), \qquad D_0D_1D_2=1.

Use Entries 762--765's complete Hom data:

eHom=(1,1,1,0,0,1,1,1,1,1,1,2),e_{\rm Hom}=(1,1,1,0,0,1,1,1,1,1,1,2),

in the ordered twelve-factor lattice

(u,v,y,1−y,1+y,v−u,y−u2,y+u2,P6,u−2,v−2,u2+1),\begin{aligned} (&u,v,y,1-y,1+y,v-u,y-u^2,y+u^2,\\ &P_6,u-2,v-2,u^2+1), \end{aligned}

and the infinity target-column shear

(w0,w1)=(0,6).(w_0,w_1)=(0,6).

Transported Gysin frame

Let PiP_i be the adapted T⊕ET\oplus E frame in chart ii. The chart filtration must not be independently reset after each occurrence move. Instead define it recursively by

Pi+1=PiDi.\boxed{P_{i+1}=P_iD_i.}

Since the raw frames obey ei=Diei+1e_i=D_i e_{i+1}, the adapted transition is

PiDiPi+1−1=1.P_iD_iP_{i+1}^{-1}=1.

Exact tests at 24 generic points give zero adapted-transition failures and zero threefold frame failures. Thus in the transported adapted frame,

AT,i+1=AT,i,AE,i+1=AE,i,Ci+1=Ci.A_{T,i+1}=A_{T,i},\qquad A_{E,i+1}=A_{E,i},\qquad C_{i+1}=C_i.

Equivalently, in arbitrary block gauges the cocycle transforms by

Ci+1=SE,i−1CiST,i.C_{i+1}=S_{E,i}^{-1}C_iS_{T,i}.

Complete pole lattice

The twelve factors are transported by chartwise pullback under the cyclic base map. Their exponent vector is retained positionally; the factors are not identified with the same fixed polynomials in every normalized chart.

Their degrees are

(1,1,1,1,1,1,2,2,4,1,1,2),(1,1,1,1,1,1,2,2,4,1,1,2),

so the complete denominator degree remains 1818. The labelled factor family and all twelve valuations return after three transports. The exact audit gives zero threefold pole-lattice failures at 24 generic points.

Rank-one defect orbit

Transporting the complete filtered splitting complex carries both its coefficient matrix and augmented cocycle column by an invertible chain isomorphism. Therefore Entry 763's one-dimensional augmented-rank cokernel has a canonical occurrence orbit:

[C12]⟼[C23]⟼[C31]⟼[C12].\boxed{ [C_{12}]\longmapsto[C_{23}]\longmapsto[C_{31}] \longmapsto[C_{12}]. }

In the recursively transported frame the three representatives are literally identical. No solver section or fitted projector is used.

This is covariance of the filtered rank-one defect. It does not upgrade Entry 763 to absolute rational nonsplitting; Entry 765's degree-thirty test and local pole stabilization remain separate obligations.

Infinity shear

The degree-six shear is a filtration on the transported (T)-lattice, not a fixed pair of ordinary-coordinate column degrees in every chart. Its rule is

Fi+1=Di−1Fi\boxed{ \mathcal F_{i+1}=D_i^{-1}\mathcal F_i }

in raw residue coordinates, or simply (0,6)(0,6) in the recursively transported adapted frame. After three steps,

F3=(D0D1D2)−1F0=F0.\mathcal F_3=(D_0D_1D_2)^{-1}\mathcal F_0=\mathcal F_0.

Thus the degree-six shear is occurrence-covariant but is not a fixed-G12G_{12} filtration imposed separately on the other charts.

Evidence

Next falsifier

Repeat Entry 765's certified degree-thirty rank tests in one transported chart and verify the four resonant graded pieces (15,17,28,30) are carried isomorphically around the cyclic orbit. Then determine local pole-order stabilization along one representative of each cyclic divisor orbit.

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