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The first connective complex K-theory Postnikov invariant is integral Sq-three

Statement

Assume AC. Write ku for Adams's connective complex K-theory spectrum bu, with its fixed Bott generator tπ2(ku)Z, and π0(ku)Z, π1(ku)=0. Its first stable Postnikov invariant is the nonzero degree-three integral operation βZSq2ρ2, where ρ2 is reduction modulo two and βZ is the integral Bockstein of 0Z2ZZ/20.

Here the stable invariant means the operation whose degree-m universal class is the first potentially nonzero space Postnikov class km+3(kum)Hm+3(K(Z,m);Z),m2, with the stage and fiber identifications fixed by the spectrum and t. The compatibility of these classes is the stable compatibility for Adams's spectrum recorded in the source input below, not a spectral assertion supplied by the definition for spaces. Its occurrence in each representing space is evaluation of this same operation; it does not assert that every evaluation is nonzero. The fixed Bott identifications transport this normalization to its coefficient rows.

Facts & Assumptions

Given: Adams's connective spectrum ku=bu and its specified Bott data as in the Statement.

[A1]

AC is assumed for the space Postnikov constructions, representability and cellular cohomology (The Axiom of Choice).

[F1]

For a connected simple space, a marked Postnikov stage with fiber K(A,n) has its class in Hn+1(Pn1X;A); this is a statement about spaces (Postnikov k-invariant, Postnikov section and Postnikov tower). For connected CW complexes, PnX can be constructed by adjoining cells of dimension at least n+2 (Postnikov towers exist for connected CW complexes). A marked simple stage is the homotopy fiber of a map representing its class (Simple Postnikov stages are classified by k-invariants).

[F2]

Positive-degree operations correspond to universal classes on K(A,m), with their positive-degree suspension identities characterized by the corresponding universal-class identities (Cohomology operations are universal classes on Eilenberg--Mac Lane spaces). Full stability requires every suspension identity, including degree zero (Stable natural cohomology operation).

[F3]

On a degree-n cocycle, Sq2 uses an2a for n2 and vanishes for n<2 (Steenrod squares from cup-i). The integral and mod-two Bocksteins have different targets and come from different coefficient sequences (Bockstein connecting operation).

[F4]

A spectrum here has weak-equivalence adjoint structure maps and stable groups are their indicated colimits (Sequential prespectra, spectra, and adjoint structure maps, Stable homotopy groups of a sequential prespectrum).

[F5]

The source computations used here are the opening of Adams, Proposition 16.6, printed p.391: the first stable invariant of bu belongs to the order-two group of degree-three stable integral operations, generated by δ2Sq2; each spectrum space has the evaluation of the same stable operation; the third space is SU; and δ2Sq2(ι3)0 in H6(K(Z,3);Z) whereas H6(SU;Z)=0. These computations and their spectrum compatibility are source inputs, not results asserted to follow from [F1] or [F2]. Adams distinguishes the mod-two Bockstein β2 on printed p.326 from the integral Bockstein δ2 on printed p.398. Thus his integral operation here is δ2Sq2ρ2=βZSq2ρ2 in the present fully typed notation. Source: https://www.sas.rochester.edu/mth/sites/doug-ravenel/otherpapers/Adams-SHGH-latex2.pdf .

[F6]

Cellular cochains compute the cohomology of a CW pair, including constant integral coefficients (Cellular cochains compute cohomology with local coefficients); the pair cohomology sequence is exact (Long exact sequence of a pair in singular cohomology).

Proof

technique · direct
1.1

We first locate the space classes correctly. For a connective Omega-spectrum, [F4] identifies πi(kum) with πim(ku) for i1: each adjoint map is a weak equivalence, so the bonding maps in that stable colimit are isomorphisms. For m2 the space is connected (its components identify with π1(kum+1)=πm(ku)=0), and it is simply connected by connectivity. Its first groups are πm=Z, πm+1=0 and πm+2=Zt. Consequently the lower space stage Pm+1kum is a K(Z,m) model. Presenting the next stage as the marked fibration of [F1], its class lies in Hm+3(K(Z,m);Z). This uses [F1] only for connected simple spaces, with n=m+2, never for a spectrum or a degree-zero space stage.

F1F4given
2.1

By [F5] the classes of step 1.1 are evaluations of a single stable operation κ and its group has just two elements: 0 and θ=βZSq2ρ2. The target types are integral to mod-two, then mod-two, then integral, respectively. [F3] supplies these local conventions; [F5], rather than [F2], supplies the stable group calculation and compatibility. In particular we are not inferring an operation group for an Eilenberg–Mac Lane spectrum from the theorem for one space K(A,m).

F2F3F5step 1.1algebra
3.1

Suppose κ=0. Its evaluation at the third space is then zero. Here Y=SU, and step 1.1 gives P4Y=K(Z,3) up to the fixed stage equivalence. The fibration P5YP4Y has fiber K(Z,5) and zero class. By [F1] it is fiber homotopy equivalent to the homotopy fiber of the constant map P4YK(Z,6), which has a section given by the constant loop. Hence H6(P4Y;Z)H6(P5Y;Z) is injective, since section pullback is its left inverse.

F1F5step 1.1step 2.1algebra
4.1

Choose the CW Postnikov model in [F1] for Y=SU. The pair (P5Y,Y) has only relative cells of dimension at least seven. Its cellular cochain group in degree six is zero, so H6(P5Y,Y;Z)=0 by [F6]. The pair sequence therefore makes H6(P5Y;Z)H6(Y;Z) injective. Composing with step 3.1 would inject the nonzero class θ(ι3) of [F5] into H6(SU;Z)=0, a contradiction. Equivalences of stage models transport these maps and do not affect injectivity.

F1F5F6step 3.1algebra
5.1

Thus κ0, and the two-element alternative of step 2.1 forces κ=θ. Its evaluation gives the stated universal class in each space by [F5]. The two identifications of an integral coefficient generator differ by sign; that sign cannot change an element of an order-two group, since θ=θ. Hence the fixed Bott identifications preserve this normalization. In low degrees evaluations may be zero: for instance Sq2 is zero on degree-zero and degree-one classes by [F3]; this illustrates why nonzero stable operation does not mean nonzero on every space. The nonvanishing used in the proof is specifically the degree-three universal class.

A1F3F5step 2.1step 4.1algebra

Source notes

The source inputs are those in Adams, Stable Homotopy and Generalised Homology, Proposition 16.6, opening on printed p.391. The full proof continues on pp.392–393 with a mod-two module calculation; that later Bockstein is not substituted for the integral one. Steps 3.1–4.1 give the missing explanation for the nonvanishing deduction using space Postnikov stages and relative cellular cohomology. Stable group classification and spectrum compatibility remain explicitly identified source computations.

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