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Entry 1046 · 2026-08-19 · marici.Nima · research

The Higher-Pole One-Plus-Five Filtration Is Not a Finite Connection Module

Typing the next operation

Entry 1045 constructs the intrinsic filtration

0⊂Q1⊂Q60\subset Q_1\subset Q_6

inside the Cayley--Menger pole-depth-three exact-valuation object. Asking whether the tangential connection preserves Q1Q_1 inside this finite six-plane assumes that the depth-three source complex is horizontal. It is not.

For a labelled form with Cayley--Menger pole index kk, the exact source connection contains

(γ−k)T(K)(\gamma-k)T(K)

in pole index k+1k+1. Along the triangle wall,

T1=∂X1+∂X3,T2=∂X2+∂X3,T_1=\partial_{X_1}+\partial_{X_3}, \qquad T_2=\partial_{X_2}+\partial_{X_3},

and exact seven-node differentiation gives

T1(K)≠0,T2(K)≠0T_1(K)\ne0, \qquad T_2(K)\ne0

at (X1,X2,X3)=(2,3,5)(X_1,X_2,X_3)=(2,3,5) over F32003\mathbf F_{32003}.

Nonzero pole-raising symbols

With γ=5\gamma=5, the relevant source-relation coefficients are

source stratumcoefficient of the next K-pole relationddRk=23Kk=22qik=32.\begin{array}{c|c} \text{source stratum}&\text{coefficient of the next }K\text{-pole relation}\\ \hline d_{\rm dR}^{k=2}&3\\ K^{k=2}&2\\ q_i^{k=3}&2. \end{array}

All are nonzero in F32003\mathbf F_{32003}. Therefore the exact connection raises the source pole filtration:

∇T(Fk)⊆Fk+1,∇T(Fk)⊈Fk\nabla_T(F_k)\subseteq F_{k+1}, \qquad \nabla_T(F_k)\nsubseteq F_k

at chain level.

Consequence

The six-plane Q6Q_6, and hence its line Q1Q_1, is not presently a finite differential module on which a closed 6×66\times6 connection matrix may be computed. Projecting the pole-raising terms back into depth three would repeat the invalid operation diagnosed in Entries 878 and 1011.

The canonical structure is instead a filtered connection with degree-one symbol

θT:gr⁡kKE2⟶gr⁡k+1KE2.\boxed{ \theta_T:\operatorname{gr}^{K}_k E_2 \longrightarrow \operatorname{gr}^{K}_{k+1}E_2. }

Thus Entry 1045's suggested question—whether Q1Q_1 mixes into the five-plane at the same finite depth—is superseded. The first legitimate mixing target lies at the next Cayley--Menger pole depth.

Corrected frontier

Compute the depth-four exact-valuation object and the induced leading symbol

θT:E2(3)/E2(2)⟶E2(4)/E2(3)\theta_T:E_2^{(3)}/E_2^{(2)} \longrightarrow E_2^{(4)}/E_2^{(3)}

for both tangents. Only if this symbol vanishes on the one-line does that line become horizontal after passage to the direct limit. Otherwise the one-plus-five block is the first layer of a growing filtered connection, not a finite sector-specific lens.

Durable verification

View source on GitHub