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LemmaStatement: Literature-sourcedProof: AI-adaptedPipeline-generatedjudge pass (gpt-5.6-terra)audited 2026-09-14
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Cartan coherence for higher diagonals

Statement

Work over F2. Put C=C∗(X), E=C∗(Y), and let A:C∗(X×Y)→C⊗E and S:C⊗E→C∗(X×Y) be Alexander--Whitney and shuffle. If T interchanges the two factors output by a higher diagonal and τ regroups

(C⊗C)⊗(E⊗E)⟶(C⊗E)⊗(C⊗E),

define degree-i maps

Li=(A⊗A)DiX×YS,Ri=∑r+s=iτ(DrX⊗TrDsY).

Let Q interchange the two C⊗E blocks. There are natural degree- (i+1) maps Hi, with H−1=0, such that

Li−Ri=dHi+Hid+(1+Q)Hi−1.

These homotopies preserve both relative carriers: for B⊆X and D⊆Y, they carry C∗(B)⊗E into (C∗(B)⊗E)⊗2 and C⊗C∗(D) into (C⊗C∗(D))⊗2.

Facts & Assumptions

Given: Spaces X,Y, their ordinary unnormalized mod-two singular chains, and a fixed natural higher-diagonal system.

[F1]

The higher diagonals satisfy dDi+Did=(1+T)Di−1 (Natural higher diagonal approximations).

[F2]

The Alexander--Whitney formula is a finite sum of tensor products of face restrictions (Alexander–Whitney map and diagonal approximation).

[F3]

The shuffle S and Alexander--Whitney A are natural chain-homotopy inverses on ordinary unnormalized chains without AC (Alexander--Whitney and shuffle are natural chain-homotopy inverses).

[F4]

A specified homotopy has a finite prism operator satisfying the singular chain-homotopy identity (The singular chain homotopy formula).

[F5]

The higher diagonals are natural (Natural higher diagonal approximations).

[F6]

The higher diagonals preserve the chain complexes of subspaces (Natural higher diagonal approximations).

Proof

technique · compare two equivariant chain maps in the same explicit fourfold acyclic carrier
1.1given

Record the diagonal on the mod-two C2 resolution. Let W have one free-orbit generator ei in every degree i≥0, with dei=(1+T)ei−1 and e−1=0. Define

ρ(ei)=∑r+s=ier⊗Tres.

With the diagonal C2 action on W⊗W, this is a chain map. Indeed, expanding dρ(ei) makes every term with r,s>0 occur twice after the index shifts (r,s)↦(r−1,s) and (r,s)↦(r,s−1); the two endpoint terms that remain are exactly ρ((1+T)ei−1). All sums are finite.

1.2F4

Fix an explicit contraction of every common fourfold model carrier. For a standard simplex Δm, let Pm be the prism from its affine contraction to the first vertex. By [F4], dPm+Pmd=1−jmpm, where pm collapses to a point and jm includes that vertex. On the unnormalized point complex, whose degree-n generator is en, put a(en)=en+1 for odd n and a(en)=0 for even n. Directly, da+ad=1−ηϵ. Hence

hm:=Pm+jmapm

satisfies dhm+hmd=1−jmηϵpm. On a tensor of four standard simplex complexes use h1⊗1⊗1⊗1+e1⊗h2⊗1⊗1+e1⊗e2⊗h3⊗1+e1⊗e2⊗e3⊗h4, where each et is its augmentation projection. The mixed terms cancel, giving a fixed h(4) with dh(4)+h(4)d=1−ηϵ. Thus every positive-degree cycle and every augmentation-zero degree-zero cycle has the specified filling h(4)z. Every displayed operator is a finite sum, so this family of contractions is fixed without AC.

2.1F1F3F5step 1.1

Assemble the two displayed families into equivariant maps. Define L(ei⊗z)=Li(z). This is the composite obtained by shuffling z to X×Y, applying the equivariant higher diagonal there, and applying A to its two outputs. Define R by first applying ρ, then applying the two higher-diagonal systems and finally regrouping with τ. The factor Tr in Ri is precisely the twist in ρ. Naturality and the chain-map identities in [F1]--[F3], together with step 1.1, show that both are C2-equivariant chain maps

W⊗(C⊗E)⟶(C⊗E)⊗2,

where C2 acts on the target by Q.

3.1step 1.2step 2.1

Construct the coherent homotopy. Induct first on i and then on p+q. Suppose Hi−1 and the values of Hi on lower-dimensional model generators are known. On the identity model generator zp,q form

ω=(Li−Ri)(zp,q)−Hi(dzp,q)−(1+Q)Hi−1(zp,q).

The chain-map equations for L and R from step 2.1 and the already established lower equations give dω=0; the two augmentation-preserving maps agree in total degree zero, so the remaining degree-zero case has augmentation zero. Set Hi(zp,q)=h(4)ω and extend to arbitrary u⊗v by postcomposition. Taking its boundary gives exactly

Li−Ri=dHi+Hid+(1+Q)Hi−1.

The postcomposition formula proves naturality. The fixed contractions and the lexicographic recursion use no choice principle.

4.1F2F3F6step 1.2step 3.1∎

The construction preserves the stated relative carriers. If u lands in B⊆X, every occurrence of u# in the two maps and in the model filling lands in C∗(B); the other factor remains in E. The same argument applies when v lands in D⊆Y. Linearity gives the assertions for their generated subcomplexes and for their sum. Empty factors give zero complexes; zero chains and i=0 are included by H−1=0; one-point and degenerate singular simplices remain in the unnormalized model. Hence every boundary case obeys the same equation.

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