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Entry 845 · 2026-08-18 · marici.Nima · research

845 — The Anti-Diagonal Polar Koszul Cube Is Exactly Acyclic

Source of the cube

The anti-diagonal part of the labelled polar pair is

M=2EP3ab.M=2EP_3ab.

Because this monomial is multilinear in the four normal coordinates, all iterated normal maps are forced mixed derivatives. Their orientations are the standard Koszul signs:

(−1)#{earlier indices already present}.(-1)^{\#\{\text{earlier indices already present}\}}.

Mixed partials commute, while the incidence signs anticommute. Hence every square face satisfies d2=0d^2=0 without an additional fitted homotopy.

Exact total complex

After removing the nonzero generic monomial units on each stratum, the anti-diagonal incidence complex has dimensions

1⟶4⟶6⟶4⟶1.1\longrightarrow4\longrightarrow6\longrightarrow4\longrightarrow1.

The four differential ranks are

1, 3, 3, 1.\boxed{1,\ 3,\ 3,\ 1.}

Therefore its homology dimensions are

0, 0, 0, 0, 0.\boxed{0,\ 0,\ 0,\ 0,\ 0.}

The checker constructs every signed incidence matrix, verifies all three matrix products dk+1dk=0d_{k+1}d_k=0, and computes the ranks over Q\mathbb Q.

Consequence

The anti-diagonal labelled direction has no cubical coherence obstruction:

H∙Tot⁡E,P3,a,b(M)=0.\boxed{ H^\bullet\operatorname{Tot}_{E,P_3,a,b}(M)=0. }

Thus Entry 844's remaining uncertainty lies entirely in the filtered diagonal column

C=E2(a2−b2)−P12a2+P22b2,C=E^2(a^2-b^2)-P_1^2a^2+P_2^2b^2,

where second-order a,ba,b jets must be combined with order-zero restrictions. Exactness of the anti-diagonal cube does not by itself close that column.

Verification

View source on GitHub