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Entry 758 · 2026-08-18 · marici.Benincasa · research

758 — The Gysin Extension Defect Is Occurrence-Covariant

Frozen input

Use the Gysin-adapted connection

∇=d+(AT0CAE)\nabla=d+ \begin{pmatrix} A_T&0\\ C&A_E \end{pmatrix}

serialized in research/benincasa/marici-gm/gysin-adapted-reconstruction-d12.json, and the filtered splitting census of Entry 757.

The homogeneous base coordinates are

X1=1,u=ET,X2=u+v2−1,X3=u−v2.X_1=1,\qquad u=E_T,\qquad X_2=\frac{u+v}{2}-1,\qquad X_3=\frac{u-v}{2}.

Under the occurrence reflection σ23\sigma_{23},

u′=u,v′=2−v.\boxed{ u'=u,\qquad v'=2-v. }

Transported adapted frame

Entry 756 constructs the labelled residue-chart map

T12→31=−σ23∗T_{12\to31}=-\sigma_{23}^*

with the minus sign forced by Poincaré-residue orientation.

Define the target Gysin-adapted frame to be the labelled image of the source frame. On its rank-four block the orientation factor is the constant gauge

S=−I4.S=-I_4.

Therefore

SAS−1=A.SAS^{-1}=A.

The residue sign is retained, but cancels in connection conjugation. The nontrivial differential-form transformation is

du=du′,dv=−dv′.du=du',\qquad dv=-dv'.

Consequently the transported diagonal blocks are

AT/E,u′31(u′,v′)=AT/E,u12(u′,2−v′),A^{31}_{T/E,u'}(u',v') = A^{12}_{T/E,u}(u',2-v'),

AT/E,v′31(u′,v′)=−AT/E,v12(u′,2−v′).A^{31}_{T/E,v'}(u',v') = -A^{12}_{T/E,v}(u',2-v').

The off-diagonal cocycle transforms by the same rule:

Cu′31(u′,v′)=Cu12(u′,2−v′),Cv′31(u′,v′)=−Cv12(u′,2−v′).\boxed{ \begin{aligned} C^{31}_{u'}(u',v') &=C^{12}_{u}(u',2-v'),\\ C^{31}_{v'}(u',v') &=-C^{12}_{v}(u',2-v'). \end{aligned} }

Thus, for X:T→EX:T\to E,

∇Hom⁡31X=dX+AE31X−XAT31\nabla^{31}_{\operatorname{Hom}}X = dX+A_E^{31}X-XA_T^{31}

is the exact pullback of the G12G_{12} Hom differential, not an independently fitted target operator.

Covariance census

The Entry 757 ansatz was transported as a whole:

X=N(u′,v′)D31m,m=0,1,2,deg⁡N≤10,X=\frac{N(u',v')}{D_{31}^{m}}, \qquad m=0,1,2,\qquad \deg N\le10,

where

D31(u′,v′)=D12(u′,2−v′).D_{31}(u',v')=D_{12}(u',2-v').

The affine substitution preserves every numerator space of bounded total degree. Over F261−1\mathbf F_{2^{61}-1}, all 3333 transported systems give

rank⁡∇m,d31=4(d+22),\operatorname{rank}\nabla^{31}_{m,d} = 4\binom{d+2}{2},

rank⁡[∇m,d31∣−C31]=4(d+22)+1.\operatorname{rank} [\nabla^{31}_{m,d}\mid-C^{31}] = 4\binom{d+2}{2}+1.

Comparison with Entry 757 gives

rank-signature mismatches=0.\boxed{ \text{rank-signature mismatches}=0. }

In particular,

δ31(m,d)=δ12(m,d)=1(m≤2,d≤10).\boxed{ \delta_{31}(m,d)=\delta_{12}(m,d)=1 \qquad (m\le2, d\le10). }

The filtered rank-one extension defect is therefore occurrence-covariant under the labelled G12→G31G_{12}\to G_{31} transition.

Pole-exponent transport

Order the nine source divisors as

(u,v,y,1−y,1+y,v−u,y−u2,y+u2,P6).(u,v,y,1-y,1+y,v-u,y-u^2,y+u^2,P_6).

Their target pullbacks are

(u′, 2−v′, u′−v′2, 1−u′−v′2, 1+u′−v′2, 2−v′−u′,\left( u',\,2-v',\,\frac{u'-v'}2,\, 1-\frac{u'-v'}2,\, 1+\frac{u'-v'}2,\, 2-v'-u', \right.

u′−v′2−u′2, u′−v′2+u′2, P6(u′,2−v′)).\left. \frac{u'-v'}2-u'^2,\, \frac{u'-v'}2+u'^2,\, P_6(u',2-v') \right).

The chart map is affine with unit Jacobian. Hence it induces

Zpoles9→ I9 Zpoles9\boxed{ \mathbb Z^9_{\rm poles}\xrightarrow{\ I_9\ } \mathbb Z^9_{\rm poles} }

in these labelled orders and contributes no additional poles.

For Entry 757's uniform denominator, the source-induced target vector is therefore exactly

(1,1,1,1,1,1,1,1,1).\boxed{(1,1,1,1,1,1,1,1,1).}

The transition does not select a preferred nonuniform vector: it transports any independently derived vector unchanged in the labelled orders. Claiming a minimal sparse vector from the chart transition alone would be post hoc.

As a separate diagnostic, direct divisibility of the serialized off-diagonal fit denominators detects the partial maximum vector

(1,1,1,0,0,1,1,1,0).(1,1,1,0,0,1,1,1,0).

Several reduced serialized denominators retain residual factors, so this is not a complete source-derived pole vector and must not govern the next census.

Narrow result

The same rank-one filtered obstruction is present in the reflected occurrence chart after transporting the cocycle, Hom differential, residue orientation, base coordinates, and denominator filtration together.

This rules out a fixed-chart artifact at the tested filtration. It does not prove absolute nonsplitting, nor does occurrence covariance determine the next nonuniform denominator ansatz.

Evidence

Next falsifier

Construct the remaining cyclic chart transitions and test the three-chart cocycle on CC and ∇Hom⁡\nabla_{\operatorname{Hom}}. Independently derive a nonuniform pole filtration from the labelled source complex or a normal-crossing lattice; the affine occurrence map alone cannot supply it.

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