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TheoremStatement: Literature-sourcedProof: AI-adaptedPipeline-generatedaudited 2026-09-22
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The first possible complex K-theory AHSS differential is integral Sq-three

Statement

Assume AC. In the complex topological K-theory Atiyah–Hirzebruch spectral sequence of Complex K-theory AHSS, the first two possible differentials are d2=0,d3=SqZ3=βZSq2ρ2, with Bott-periodic translates of this formula on all even coefficient rows. Here ρ2 is reduction modulo two, Sq2 is the Steenrod square and βZ is the integral Bockstein of 0Z2ZZ/20; the operation is defined on integral cohomology by SqZ3=βZSq2ρ2:Hn(X;Z)Hn+3(X;Z).

Facts & Assumptions

[A1]

Assume AC. For a finite CW complex the K-AHSS has E2p,q=Hp(X;Z) for even q, E2p,q=0 for odd q, and dr:Erp,qErp+r,qr+1 (Complex K-theory AHSS).

[A2]

Under the K-AHSS, for p1 the differential d3 is read from the relevant kp+3 Postnikov layer of the total-degree representing space kup+q; after Bott translation to a nonpositive coefficient row, this is the stable operation βZSq2ρ2 (KU representability and the skeletal–Postnikov d-three comparison, The first connective complex K-theory Postnikov invariant is integral Sq-three).

[A3]

Steenrod squares vanish above the degree: for xHn(X;F2) one has Sqkx=0 when k>n, so in particular Sq2(ρ2y)=0 for yH0(X;Z) (Steenrod normalization, instability, suspension, and top square, Steenrod squares from cup-i).

[A4]

A finite CW complex has finitely many path components, each a connected finite CW complex with H0(Xa;Z)=Z. Naturality gives restriction maps of the K-AHSS along the component inclusions (Naturality and edge maps of the AHSS).

[A5]

Bott periodicity gives natural isomorphisms Kq(X)Kq2(X) and identifies all even coefficient rows with the row K0()=Z (Complex Bott periodicity).

Proof

technique · direct

Given: Assume AC, a finite CW complex X, and the K-AHSS of [A1].

1.1

The differential d2 has bidegree (2,1): it maps the even coefficient row q to the odd row q1, which is zero by the coefficient computation; hence d2=0 and E3=E2.

A1A5given
1.2

Let X=a=1mXa be the finite decomposition into connected components. On each Xa, every class of H0(Xa;Z)=Z is pulled back from the point, so naturality identifies its d3 with the pullback of d3 on the point; the latter has target H3(pt;Z)=0. For yH0(X;Z), naturality along XaX therefore makes every restriction of d3yH3(X;Z) zero. Every singular simplex of a disjoint union lies in one component, so restriction gives an isomorphism of singular cochain complexes C(X;Z)a=1mC(Xa;Z) and hence an injective map H3(X;Z)aH3(Xa;Z). Thus d3y=0 without assuming a componentwise decomposition of the entire AHSS.

A1A4given
1.3

For p1 and any even coefficient row, the comparison and k-invariant lemmas identify d3 on E3p,q with βZSq2ρ2, transported along the Bott identification of the coefficient rows.

A2A5given
2.1

On the p=0 row the operation βZSq2ρ2 also vanishes, since Sq2 is zero on classes of degree zero by instability; thus the formula d3=βZSq2ρ2 holds on the p=0 row as well.

A3step 1.2
3.1

Combining steps 1.1, 1.3 and 2.1 gives d2=0 and d3=βZSq2ρ2 on every even coefficient row, with the Bott-periodic translates supplied by [A5]; the sign ambiguity of the long exact sequence convention is immaterial because the operation has order two.

A5step 1.1step 1.3step 2.1
4.1

step 3.1 proves the asserted vanishing of d2 and the identification of d3 with SqZ3=βZSq2ρ2 on all even coefficient rows.

step 3.1

Source notes

Compare Ji, Proposition 3.12, printed p. 12, for the statement d3=Sq~3 and the description of the operation as the composite of reduction mod two, Sq2 and the integral Bockstein; the normalization of the operation is supplied by Adams, Proposition 16.6, printed pp. 391–393.

Depends on

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