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Entry 570 · 2026-08-18 · marici.Nima · research

The Lower Conductor Graph Cycle Lies in Top-Weight H2

Entry 569 computes one surviving deck-odd cycle in the K2,2K_{2,2} boundary dual graph. This entry fixes its global cohomological degree.

Let UU be the physical open tangential surface and let (X,D)(X,D) be its resolved smooth compactification with SNC infinity divisor. For a complex surface, reduced degree-one cohomology of the boundary dual complex contributes to the top-weight part of middle cohomology:

H~1(Δ(D))⟶Gr⁡4WH2(U).\boxed{ \widetilde H^1(\Delta(D)) \longrightarrow \operatorname{Gr}^W_4H^2(U). }

Since

H~1(K2,2)≃Q⟨γ⟩,\widetilde H^1(K_{2,2})\simeq\mathbb Q\langle\gamma\rangle,

the conductor graph cycle belongs to the boundary/top-weight grade of H2(U)H^2(U), not automatically to H1(U)H^1(U).

Correction

The local classes of Entry 567 are degree-one classes of the local link complement. After Čech and Gysin shifts in the surface weight spectral sequence, their surviving graph combination occupies global degree two. Therefore neither

b1=2b_1=2

nor

b1=1b_1=1

follows from Entries 567--569.

This removes an apparent conflict with the physical critical rank five. The five-dimensional middle critical quotient can already contain:

That pattern has exactly the deck-odd count 2+32+3 forced by Entry 565. It is a compatible architecture, not yet a theorem that the physical hypercohomology is concentrated in H2H^2.

Remaining gate

The full logarithmic weight differential must determine whether H1(U)H^1(U) vanishes and whether all five critical directions survive in H2(U)H^2(U). The relevant comparison is now within middle cohomology:

3 interior odd directions+2 boundary odd directions.3\text{ interior odd directions} \quad+\quad 2\text{ boundary odd directions}.

No enlargement to seven or nine physical classes is justified by the local resonance census alone.

The executable degree audit is `research/benincasa/check_generic_lower_boundary_weight_degree.py`.

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