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Generalized Cohomology and the Atiyah Hirzebruch Spectral Sequence

1 · Prerequisites

2 · Summary

A reduced generalized cohomology theory is fixed axiomatically: homotopy invariance, exact cofiber sequences with suspension isomorphisms, and the wedge axiom, with no dimension axiom. The same page records the covariant homology axioms separately, because the homological AHSS is not obtained by reversing the cohomological arrows. Coefficient groups are the reduced groups of S0 in each degree, and on spheres the degree of a self-map acts as multiplication on every generalized group.

For a finite CW complex the skeletal filtration and its exact couple produce both forms of the Atiyah–Hirzebruch spectral sequence. The first page is cellular cochains or chains with theory coefficients, the first differential is the cellular (co)boundary, and the second page is ordinary (co)homology with coefficients in the graded coefficient group. Convergence is stated for finite CW complexes only: finite dimension bounds the skeletal index and no hypothesis is placed on the coefficient index, so edge maps remain the structural maps of the exact couple even when the coefficient rows extend infinitely in both directions. Naturality holds for arbitrary CW maps through cellular approximation, and for theory morphisms commuting with suspension and connectors.

A coherent external product makes the spectral sequence multiplicative: page algebras, derivation differentials, multiplicative filtration and the associated-graded ring at the stable page. Collapse is kept separate from extension data, and the page ends with the complex K-theory application: the K-AHSS has d2=0 and d3=βZSq2ρ2, obtained from the Bott-compatible representing spectrum, its connective cover and the first Postnikov invariant of the ku representing spaces.

3 · Logical flowchart

4 · Definitions, theorems and proofs

DefinitionDefinition: Literature-sourcedProof: Not applicableaudited 2026-09-22Open item page →

Reduced generalized cohomology theory

Definition

A reduced generalized cohomology theory on based CW complexes consists of the following data.

  1. For every integer n a contravariant functor h~n from based CW complexes and based cellular maps to abelian groups; a based cellular map f:XY induces f:h~n(Y)h~n(X).
  2. For every based CW complex X and integer n a suspension isomorphism σ=σn(X):h~n(X)  h~n+1(ΣX), natural in X, where Σ is the reduced suspension and the sphere coordinate is written first.

For every based cellular map f:XY, use the cofiber convention of Reduced cone suspension and cofiber sequence: XfYiCfqfΣX. The connecting homomorphism is normalized by the suspension and is not independent structure:

δf:=qfσn(X):h~n(X)h~n+1(Cf).

Thus its sign is fixed by the displayed cofiber sequence, the convention that the suspension coordinate is written first, and the chosen suspension isomorphism.

The data satisfy the following axioms.

  • (H) Homotopy invariance. If fg are based homotopic based maps, then f=g on every reduced group.
  • (E) Exactness. For every based cellular map f:XY the sequence h~n(Cf)ih~n(Y)fh~n(X)δfh~n+1(Cf) is exact. The normalized connecting maps are natural for maps of based maps because the collapse maps qf and the suspension isomorphisms are natural.
  • (W) Wedge axiom. For every family (Xα) of based CW complexes and every n the natural map h~n(αXα)αh~n(Xα) induced by the summand inclusions is an isomorphism. For a finite index set the product is the direct sum; the empty wedge is a point and the empty product is the zero group, so in particular h~n()=0.

No dimension axiom is imposed: the value h~n(S0) is an arbitrary abelian group, called the coefficient group of degree n; the coefficient bookkeeping is recorded by the coefficient-groups definition on this page. Ordinary reduced singular cohomology with coefficients in an abelian group is the special case in which the dimension axiom holds, and the whole point of the definition is to admit theories for which h~n(S0) is nonzero in infinitely many degrees. A morphism of reduced generalized cohomology theories is a family of natural transformations commuting with the suspension isomorphisms. It then commutes with every connecting map because δf=qfσ.

Source notes

Compare Loizides, §2, printed pp. 3–4, for the homotopy, wedge and exactness axioms, the suspension isomorphism hnΣhn1 and the definition hn:=hn(S0)=hn(pt) of the coefficient groups. In the paragraph ending on printed p. 3, the pair boundary is explicitly the suspension isomorphism followed by pullback along the cofiber-to-suspension map; this is the normalization imposed above. Davis--Kirk, §8.8, gives the corresponding reduced/unreduced axioms and correspondence.

DefinitionDefinition: Literature-sourcedProof: Not applicableaudited 2026-09-22Open item page →

Reduced generalized homology theory

Definition

A reduced generalized homology theory on based CW complexes consists of the following data.

  1. For every integer n a covariant functor h~n from based CW complexes and based continuous maps to abelian groups; a based map f:XY induces f:h~n(X)h~n(Y).
  2. For every based CW complex X and integer n a suspension isomorphism σ=σn(X):h~n(X)  h~n+1(ΣX), natural in X.
  3. For every based cellular map f:XY, write Cf for its reduced cofiber, i:YCf for the structural inclusion and qf:CfΣX for the cofiber map. The connecting homomorphism is required to be the composite f:=σn(X)1(qf):h~n+1(Cf)h~n(X). Thus it is natural in f and lowers the homological degree by one; it is not independent extra data that may be normalized separately from suspension.

The data satisfy the following axioms.

  • (H) Homotopy invariance. Based homotopic maps induce equal homomorphisms.
  • (E) Exactness. For every based cellular map f:XY the long sequence h~n(X)fh~n(Y)ih~n(Cf)fh~n1(X) is exact. Its connecting maps have the suspension-compatible normalization in item 3 and are natural for commutative squares of based cellular maps. (The cellular restriction ensures that Cf is again a based CW complex, hence is an object in the declared domain of the functors.)
  • (W) Wedge axiom. For every family (Xα) of based CW complexes and every n the natural map αh~n(Xα)h~n(αXα) induced by the summand inclusions is an isomorphism. The empty wedge is a point and the empty sum is the zero group, so h~n()=0.

No dimension axiom is imposed: h~n(S0) is an arbitrary abelian group. A generalized homology theory is a genuinely covariant notion: it is not obtained by reversing the arrows of Reduced generalized cohomology theory, and the two notions are logically independent apart from the common coefficient bookkeeping recorded in Coefficient groups of a generalized homology theory. A morphism of reduced generalized homology theories is a family of natural transformations commuting with suspension and the connecting maps.

Source notes

Compare Davis–Kirk, Definition 8.27, printed pp. 227–229, for the reduced homology axioms on based CW complexes. Their exactness axiom is the three-term cofiber exactness axiom; iterating the cofiber sequence with their suspension isomorphism gives the long sequence above and fixes its boundary as (qf) followed by inverse suspension. Definition 8.28 gives the coefficient groups used in Coefficient groups of a generalized homology theory.

DefinitionDefinition: Literature-sourcedProof: Not applicableaudited 2026-09-22Open item page →

Coefficient groups of a generalized cohomology theory

Definition

Let h~ be a reduced generalized cohomology theory on based CW complexes in the sense of Reduced generalized cohomology theory. Its coefficient group in degree qZ is hq():=h~q(S0), where S0={0,1} is based at 1. Equivalently, if h is the pair theory associated with h~ by Reduced and unreduced generalized cohomology theories correspond, then h~q(S0)=hq(pt): the coefficient group is the value of the unreduced theory on a point.

The suspension isomorphisms of the theory identify the reduced groups of spheres in all degrees. Composing the isomorphisms h~np(S0) σ h~np+1(S1) σ  σ h~n(Sp) gives, for every p0 and every nZ, a canonical isomorphism h~n(Sp)hnp(). For p=0 this is the identity h~n(S0)=hn(). These identifications are compatible with the iterated suspension maps used to construct them. An arbitrary based self-map of a sphere need not act as the identity under these identifications; its induced endomorphism is transported to the corresponding endomorphism of the coefficient group. No dimension axiom is imposed, so the groups hq() may be nonzero for infinitely many q.

Source notes

Compare Loizides, §2, printed p. 3, for the convention hn:=hn(S0)=hn(pt) and Remark 2.2 together with the wedge axiom for the resulting product decompositions.

DefinitionDefinition: Literature-sourcedProof: Not applicableaudited 2026-09-22Open item page →

Coefficient groups of a generalized homology theory

Definition

Let h~ be a reduced generalized homology theory on based CW complexes in the sense of Reduced generalized homology theory. Its coefficient group in degree qZ is hq():=h~q(S0), where S0={0,1} is based at 1. Equivalently, if h is the pair theory associated with h~, then h~q(S0)=hq(pt).

Composing the homological suspension isomorphisms h~np(S0) σ h~np+1(S1) σ  σ h~n(Sp) gives, for every p0 and every nZ, a canonical isomorphism h~n(Sp)hnp(). For p=0 this is the identity h~n(S0)=hn(). The homological coefficient groups of a sphere are therefore read in the same degree-shifted way as the cohomological coefficient groups; the covariant theory itself is defined separately in Reduced generalized homology theory. No dimension axiom is imposed.

Source notes

Compare Davis–Kirk, Definition 8.28, printed pp. 229–230, for the coefficient groups hn()=hn(S0) of a reduced generalized homology theory.

PropositionStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

Reduced and unreduced generalized cohomology theories correspond

Statement

Call a CW-pair cohomology theory a contravariant functor h on CW pairs (X,A) with a CW subcomplex AX and cellular maps of pairs, taking values in abelian groups hn(X,A) for nZ, together with natural connecting homomorphisms :hn(A)hn+1(X,A) such that:

  • (H) homotopic maps of pairs induce equal maps;
  • (LES) for every CW pair the sequence hn(X,A)hn(X)hn(A)hn+1(X,A) is exact, where hn(X):=hn(X,);
  • (Ex) if U,VX are subcomplexes with X=UV, the inclusion induces hn(U,UV)hn(X,V);
  • (Add) for every set-indexed family of CW pairs the inclusions induce αhn(Xα,Aα)hn(αXα,αAα), the empty family giving the zero group.

No dimension axiom is imposed. Then reduced generalized cohomology theories on based CW complexes in the sense of Reduced generalized cohomology theory and CW-pair cohomology theories determine one another, naturally and compatibly with morphisms, through the following two constructions.

(A) Given a reduced theory h~, put, for a CW pair (X,A), hn(X,A):=h~n(Ci), where i:A+X+ is the based inclusion and Ci is its reduced cofiber. Equivalently hn(X,)=h~n(X+) and, for A, hn(X,A)h~n(X/A), the quotient based at the collapsed subcomplex. In particular hn(X)=h~n(X+). The connecting homomorphism of the pair (X,A) is the connecting map of the cofiber sequence of i.

(B) Given a CW-pair theory h, put, for a based CW complex Y whose basepoint is a vertex, h~n(Y):=hn(Y,). The suspension isomorphism is the connecting map of (CY,Y) restricted to hn(Y,), followed by the quotient identification and suspension reflection: σ=ρYκY1:hn(Y,)hn+1(ΣY,), where κY:hn+1(ΣY,)hn+1(CY,Y) is quotient pullback and ρY([y,t])=[y,1t]. The reflection is required by the fixed cone coordinate convention, as checked below. For a based cellular map f:XY, its reduced connector is then δf=qfσ, where qf:CfΣX is the collapse in the fixed reduced cofiber sequence.

In all quotient formulas use the based convention X/:=X+; when A is nonempty, X/A is the usual collapsed quotient.

The two constructions are canonically inverse: for a reduced theory h~ the theory obtained by (B) from the theory built in (A) satisfies h~n(Y)hn(Y,)h~n(Y), and for a CW-pair theory h the theory built in (A) from that obtained by (B) satisfies hn(X,A)h~n(X/A)hn(X,A). Under these identifications the connecting maps agree. In particular the three displayed formulas hn(X,A)=h~n(X/A), h~n(Y)=hn(Y,) and hn(X)=h~n(X+) hold with all structure maps transported.

Facts & Assumptions

[F1]

A reduced generalized cohomology theory consists of contravariant functors on based CW complexes and natural suspension isomorphisms σ:h~n(X)h~n+1(ΣX) satisfying (H), (E) and (W); for the fixed cofiber sequence XfYCfqfΣX, its connector is normalized as δf=qfσ (Reduced generalized cohomology theory).

[F2]

A CW subcomplex inclusion is a cofibration, and the reduced cofiber of the based inclusion A+X+ is the space XACA (Relative CW inclusions are cofibrations, Reduced cone suspension and cofiber sequence).

[F3]

For a based cofibration i:AX the collapse CiX/A is a based homotopy equivalence (Cofiber of a based cofibration is equivalent to the quotient).

[F4]

For a CW pair (X,A) with A, the quotient X/A is a CW complex with one vertex replacing A and one cell per cell of XA (CW quotients and collapse of a contractible subcomplex).

[F5]

The wedge of based spaces is the quotient of their disjoint union identifying all basepoints; a disjoint union of based spaces whose basepoints are identified with one new point is the wedge of the based spaces (The wedge of a family of pointed spaces).

[F6]

The five lemma compares exact sequences of abelian groups when the four surrounding maps are isomorphisms (The Five Lemma for modules).

Proof

technique · direct

Given: A reduced theory h~ and a CW-pair theory h as in the statement; all CW pairs have supplied characteristic maps and all based spaces are based at vertices.

1.1

First record two consequences of the pair axioms, for use in construction (B). The sequence of (Z,Z) gives hn(Z,Z)=0: the adjacent maps hn(Z)hn(Z) are identities. For a based complex Z, the retraction Z splits hn(Z)hn(). Thus the sequence of (Z,) identifies hn(Z,) naturally with its kernel and gives hn(Z)=hn(Z,)hn(). For a based subcomplex DZ, remove the split point summands from the pair sequence to obtain the exact sequence hn(Z,D)hn(Z,)hn(D,)hn+1(Z,D). Indeed the pair boundary kills the point summand because it is in the image of hn(Z).

givenalgebra
1.2

The quotient axiom for a pair theory follows from the stated axioms, rather than being an additional assumption. For nonempty DZ, form T=ZDCD, where CD here is the ordinary cone with its tip as basepoint; equivalently it is the reduced cone on D+. The collapse TZ/D is a homotopy equivalence by [F2] and [F3]. Its restriction CD is also a homotopy equivalence. The natural pair sequences and [F6] therefore make hn(Z/D,)hn(T,CD) an isomorphism. Excision for the subcomplex cover T=ZCD makes hn(T,CD)hn(Z,D) an isomorphism. Their composite is precisely the pullback of the quotient map of pairs (Z,D)(Z/D,), so this identification is natural. For D=, additivity identifies hn(Z+,) with hn(Z,). This proves the same assertion with the stipulated convention Z/=Z+.

F2F3F4F6given
1.3

Starting with a reduced theory, define hn(X,A)=h~n(CA+X+). Maps and homotopies of pairs induce maps and homotopies of these cofibers, proving functoriality and (H). Cofibration collapse identifies the cofiber with X/A when A. For A=, A+ is a point, and its reduced cone adds nothing to X+, so the cofiber is X+. In all cases the cofiber exact sequence gives (LES), with boundary qiσ.

F1F2F3
2.1

For subcomplexes X=UV, the map U/(UV)X/V is a based homeomorphism under the empty-quotient convention. If UV is empty and V is nonempty, the collapsed V is the adjoined isolated basepoint of U+; if V is empty both quotients are X+. In the remaining case both quotients have the same cell characteristic maps and weak topology. This proves (Ex). Also (Xα)+=(Xα)+, including an empty family, and the cofiber of the wedge of these inclusions is the wedge of their cofibers, by their explicit quotient constructions. The reduced wedge axiom proves (Add).

F1F2F4F5step 1.3
2.2

Conversely set h~n(Y)=hn(Y,). This is a homotopy-invariant functor and is zero at a point by step 1.1. For the reduced cone pair (CY,Y), step 1.1 and based contractibility of CY give an isomorphism :hn(Y,)hn+1(CY,Y). By step 1.2 the quotient map induces an isomorphism κY:hn+1(ΣY,)hn+1(CY,Y). Define σ=ρYκY1 as in (B). All these maps are natural, so this is a natural suspension isomorphism.

F2step 1.1step 1.2
2.3

For the wedge axiom, form a CW complex Z from the disjoint union of the Yα by adjoining one new vertex and an interval from it to each supplied basepoint. Let T be the union of those intervals and their endpoints. The simultaneous linear contraction of the intervals to the new vertex contracts T; it is continuous in the CW weak topology. The quotient Z/T is the wedge with its CW topology. Excision for the subcomplex cover by T and Yα, and then (Add), give hn(Z,T)hn(Yα,{α})hn(Yα,α). Step 1.2 identifies the left side with hn(Yα,). The comparison is the map induced by summand inclusions, since all the quotient and excision maps restrict to those inclusions. For the empty family Z=T= and all groups are zero. Thus (W) holds.

F4F5step 1.1step 1.2given
3.1

To check the connector including its sign, use the reduced mapping cylinder Mf=Yf(X×I), attaching X×{0} to Y and collapsing the basepoint track. Its free end X×{1} is a CW subcomplex, Mf retracts onto Y, and Mf/(X×{1})=Cf with the cone coordinate of [F2]. Define a map of pairs (Mf,X×{1})(CX,X×{0}) by sending Y to the cone tip and [x,t] to [x,1t]. It is the identity on the identified copies of X. On quotients it induces ρXqf:CfΣX. Naturality of the pair boundary and the quotient isomorphisms of step 1.2 now identify the cylinder boundary on hn(X,) with (ρXqf)κX1=qfσ. The reduced pair sequence of step 1.1, together with the retraction, is exactly (E), with this connector. This proves both exactness and the normalization required by [F1].

F1F2step 1.1step 1.2step 2.2
4.1

Starting from a reduced theory, applying (A) and (B) yields hn(Y,)=h~n(CS0Y+)h~n(Y+/S0)=h~n(Y); this is natural, not a claimed decomposition of Y+. Check suspension as well. The cofiber of YCY is two reduced cones glued along their bases. Collapsing the attached cone gives the quotient model CY/Y=ΣY, whereas the cofiber-to-suspension map collapses the first cone. These two maps differ, up to based homotopy, by reflection of the suspension coordinate: parametrize it by s[0,2] from the first tip through the equator at 1 to the second tip. If ψ collapses the attached cone, then ρψ is [y,s][y,min(s,1)], and q is [y,s][y,max(s1,0)]. The maps [y,s][y,min(1,max(0,sa))] for 0a1 give the required based homotopy. Consequently the cone-pair boundary transported to ΣY is ρYσoriginal. The additional reflection in (B) cancels this, since ρY2=id. Thus the recovered suspension is the original one. All cofiber connectors then agree because both are qfσ.

F1F2F3step 2.2step 3.1
4.2

Starting from a pair theory, (B) followed by (A) gives hn(X,A)=hn(Ci,). Cofibration collapse and step 1.2 identify this naturally with hn(X,A), including A=. To check boundaries, replace A+X+ by its reduced mapping cylinder. The cylinder collapse is a map of pairs to (X+,A+), an ordinary homotopy equivalence on total spaces and the identity on the identified copies of A+. Naturality of the pair sequences and the five lemma make its relative pullback an isomorphism. Additivity identifies the latter relative and absolute maps with those for (X,A). The coordinate calculation of step 3.1 identifies its connecting map under the quotient comparison with qiσ. Hence the pair boundary recovered by (A) is the original one, with its sign. The same constructions commute with morphisms of theories, since they use only pullbacks, boundaries and inverses of natural isomorphisms.

F1F2F3F6step 1.2step 3.1
5.1

The two natural comparisons of steps 4.1 and 4.2 preserve all structure maps and give the asserted inverse constructions. Empty spaces and empty subcomplexes use X/=X+, points have zero reduced groups, and no dimension axiom or coefficient restriction has entered. No family of arbitrary choices is used: cones, cylinders, quotients and the interval contraction are specified constructions on the supplied CW data.

step 2.1step 2.3step 4.1step 4.2

Source notes

Compare Davis–Kirk, §8.8, printed pp. 227–233, for the pair long exact sequence, the reduced homology/cohomology axioms and the quotient presentation hn(X,A)h~n(X/A); and Loizides, §2, printed pp. 3–4, for the reduction h~n(X)=ker(hn(X)hn(pt)) and the pair long exact sequence obtained from the cone sequence.

PropositionStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

Degree-d sphere maps act by multiplication by d in any generalized theory

Statement

Give Sp for p1 its CW structure with the basepoint as sole vertex and one p-cell, and give finite wedges the corresponding wedge structure. Let p1, let f:SpSp be a based continuous map of degree dZ in the sense of Degree of a self map of an oriented sphere, and let h~ be a reduced generalized homology theory (Reduced generalized homology theory) and g~ a reduced generalized cohomology theory (Reduced generalized cohomology theory) on based CW complexes. Then f:h~n(Sp)h~n(Sp),f:g~n(Sp)g~n(Sp) are multiplication by d for every integer n. For p=0 the only based self-maps of S0 (with its discrete CW structure) are the identity and the collapse map, and they induce identity and zero respectively. If one calls these integers their degrees, this uses reduced H0(S0;Z)Z, not the unreduced positive-dimensional definition cited above.

Facts & Assumptions

[F1]

For r1, degree is an isomorphism πr(Sr,b)Z sending the identity to 1; the group operation is the oriented pinch sum, equivalently cubical concatenation, and two based self-maps of Sr are based homotopic if and only if their degrees agree (Based sphere maps are classified by degree).

[F2]

For p1, homological degree is defined by f[Sp]=d[Sp] in Hp(Sp;Z)Z (Degree of a self map of an oriented sphere).

[F3]

A reduced generalized homology theory has based homotopy invariance, and for a finite wedge the summand inclusions induce an isomorphism αh~n(Xα)h~n(αXα) (Reduced generalized homology theory).

[F4]

A reduced generalized cohomology theory has based homotopy invariance, and for a finite wedge the summand inclusions induce an isomorphism g~n(αXα)αg~n(Xα) (Reduced generalized cohomology theory).

[F5]

The wedge is the quotient of the disjoint union of the summands identifying their basepoints, and the structural maps of a wedge are the summand inclusions and collapses (The wedge of a family of pointed spaces).

[F6]

Integral singular homology is homotopy invariant and computed naturally by cellular chains; the reduced sphere groups have their usual generator, including reduced H0(S0)=Z (Homotopic maps induce the same map on singular homology, Cellular homology computes singular homology, Homology of spheres).

Proof

technique · direct

Given: A based degree-d map f:SpSp, p1, and a reduced homology theory h~ and reduced cohomology theory g~.

1.1

All maps used are in the functors' domains. For p1 the skeleton of Sp in each dimension 0k<p is its basepoint and in dimensions kp is the entire sphere. The same description holds for a finite wedge with its common vertex. Every based continuous map among these spaces therefore preserves every skeleton and is cellular. For p=0 every map of the discrete vertex sets is cellular. In particular this applies to f, pinch, fold, wedge inclusions, collapses and wedge maps; the homotopy axiom applies to based homotopies between these cellular endpoints. Let r be the geometric degree in [F1]. Then [f]=r[id] under pinch addition. We compare r with the homological degree d below.

F1F3F4given
1.2

Write P:SpSpSp for the pinch and F:SpSpSp for the fold, so that for based self-maps α,β the pinch sum is represented by F(αβ)P; the two components π1P,π2P are based degree-one maps, hence are based homotopic to the identity.

F1F5given
1.3

For p=0 the only based self-maps are identity and collapse. Identity induces identity by functoriality; collapse factors through a point, whose reduced groups are zero by the empty-wedge clauses of [F3] and [F4], so it induces zero. These are also the integers acting on reduced H0(S0;Z) by [F6]. No degree is defined here using unreduced H0(S0;Z)Z2.

F3F4F6
2.1

For homology, P:h~n(Sp)h~n(SpSp) has components (π1P)=(π2P)=id under the wedge isomorphism of [F3], hence is the diagonal; and F is the sum map because F restricts to the identity on each summand. Therefore (F(αβ)P)=α+β for all based α,β.

F3F5step 1.2
2.2

For cohomology, F is the diagonal and P is the sum map under the wedge isomorphism of [F4], because F restricts to the identity on each summand and the components of P are degree one; therefore (F(αβ)P)=α+β for all based α,β.

F4F5step 1.2
3.1

By step 1.1 and functoriality of h~, f equals the r-fold sum of id in the group End(h~n(Sp)), which is multiplication by r by step 2.1. For negative r, an inverse class has the negative induced map, since adding it to the original class gives a nullhomotopic map, which factors through the zero reduced group of a point. The same observation includes r=0.

F3step 1.1step 2.1
3.2

By step 1.1 and functoriality of g~, f equals the r-fold sum of id in the group End(g~n(Sp)), which is multiplication by r by step 2.2, including r<0: the additive inverse class induces the negative endomorphism since its pinch sum with the original is null and hence induces zero through a point.

F4step 1.1step 2.2
3.3

The same finite pinch calculation in ordinary integral homology identifies the two degree conventions. By [F6], the top homology of a finite wedge of p-spheres is free on the sphere inclusions: its cellular complex has a common vertex, one generator per p-cell, and zero boundary (also for p=1, since both endpoints attach to that vertex). The collapses give the corresponding coordinate projections. Thus pinch is diagonal and fold is addition in top homology, exactly as in step 2.1. Homotopy invariance [F6] and [f]=r[id] give f[Sp]=r[Sp]. By the definition [F2], d=r.

F2F6step 1.1step 2.1
4.1

Combining steps 1.3, 3.1 and 3.2 gives the asserted multiplication by the degree on every reduced homology and cohomology group of Sp.

step 1.3step 3.1step 3.2step 3.3

Source notes

Compare Loizides, Lemma 2.3 and Remark 2.2, printed pp. 4–5, where the degree action is proved for cohomology by factoring a positive-degree map through a pinch to a wedge followed by a folding map, with its negative-degree case left to a similar trick. Here pinch additivity proves the inverse-class action explicitly, and the ordinary cellular homology calculation identifies geometric and homological degrees.

DefinitionDefinition: Literature-sourcedProof: Not applicableaudited 2026-09-22Open item page →

Skeletal filtration for generalized cohomology

Definition

Let X be a finite CW complex with skeleta Xp, and let h be the CW-pair cohomology theory associated with a reduced generalized cohomology theory h~ by Reduced and unreduced generalized cohomology theories correspond. Use the conventions Xp=(p<0),Xp=X(pdimX), so that X1=. The skeletal filtration of hn(X) is the decreasing filtration Fphn(X):=ker(hn(X)hn(Xp1)),pZ.

By the long exact sequence (LES) of the pair (X,Xp1) and the fact that a relative group maps onto the kernel of the restriction, the same subgroup is Fphn(X)=im(hn(X,Xp1)hn(X)), the image being the kernel of the next restriction by exactness. The filtration is decreasing, Fp+1hn(X)Fphn(X), because the restriction to Xp1 factors through the restriction to Xp. For a finite CW complex it is bounded and exhaustive: Fphn(X)=hn(X) for p0, since hn()=0, and Fphn(X)=0 for p>dimX, since then Xp1=X and the restriction is the identity. No completeness or infinite dimension is asserted.

Source notes

Compare Loizides, §3, printed pp. 4–7, where for a finite CW complex the filtration is written Fmhn(X)=ker(hn(X)hn(Xm)), the indexing here being shifted by one so that Fphn(X) corresponds to the classes vanishing on the (p1)-skeleton; see also Theorem 3.4 and Remark 3.5 there.

LemmaStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

The AHSS E-one page is cellular cochains with theory coefficients

Statement

Let X be a finite CW complex with supplied characteristic maps and cell orientations, and let h~ be a reduced generalized cohomology theory. Use the associated cofiber model for relative groups: hr(B,A):=h~r(CA+B+), where + adjoins a disjoint basepoint. Thus hr(B,)=h~r(B+) and the coefficient group is hq()=h~q(S0). Set Xp= for p<0. The first skeletal groups E1p,q=hp+q(Xp,Xp1) have natural isomorphisms E1p,qCcellp(X;hq()):=Hom(Cpcell(X;Z),hq()) for all integers p,q. In particular these identify the first page of the skeletal exact couple whenever h is given as its CW-pair theory with this cofiber model. This assertion uses only these relative groups, not an equivalence between categories of theories.

The isomorphisms commute with cellular maps through their induced cellular chain maps, and with morphisms of reduced theories through the induced coefficient homomorphisms. Orientations fix the cell coordinates; a reversal of a chosen cellular generator reverses the corresponding coefficient coordinate.

Facts & Assumptions

Given: The stated finite CW data, h~, and the displayed relative-group convention.

[F1]

CW subcomplex inclusions are cofibrations; the reduced cofiber of a based cofibration maps by a based homotopy equivalence to the quotient (Relative CW inclusions are cofibrations, Cofiber of a based cofibration is equivalent to the quotient, Reduced cone suspension and cofiber sequence).

[F2]

Collapsing a nonempty CW subcomplex retains a vertex for that subcomplex and the remaining cells, with their quotient characteristic maps; the empty wedge is a point (CW quotients and collapse of a contractible subcomplex, The wedge of a family of pointed spaces).

[F3]

The reduced functors are homotopy invariant and satisfy the wedge axiom by summand restrictions; the point has zero reduced groups. Their natural suspension isomorphisms identify h~p+q(Sp) with hq() for p0 (Reduced generalized cohomology theory, Coefficient groups of a generalized cohomology theory).

[F4]

Cellular chains in degree p0 are the relative homology of consecutive skeleta and are free on their oriented p-cells; they vanish for p<0 (Oriented cellular chain group, Relative homology of consecutive CW skeleta).

[F5]

For p1, degree classifies based sphere self-maps, is an isomorphism πp(Sp)Z, sends identity to 1, and sends oriented pinch sum to addition (Based sphere maps are classified by degree).

Proof

technique · direct
1.1

If X=, all skeletal pairs are (,). Their based cofiber is the cofiber of , hence a point, and [F3] gives E1p,q=0 for every p,q. There are no cells, so [F4] gives the zero Hom group. For any X and p<0 the same argument applies. These cases are settled without taking the unbased quotient /.

F1F3F4given
1.2

Suppose now X and p0. For p=0, the cofiber of X+0 is X+0 itself, which is the finite wedge of one S0 for each vertex. For p1, Xp1 is nonempty since X has a vertex. By [F1] the cofiber of X+p1X+p is based homotopy equivalent to X+p/X+p1=Xp/Xp1. This is a wedge of p-spheres: each supplied characteristic disk has its whole boundary collapsed to the single quotient vertex, and the quotient CW topology of [F2] is exactly the wedge topology. If there are no p-cells the quotient is a point. All comparisons commute with the quotient maps induced by cellular maps.

F1F2given
1.3

We verify the degree action needed for cellular naturality directly. For p1 let P:SpSpSp be the oriented pinch and r1,r2 its two collapse projections. Each riP is homotopic to identity (shrink the collapsed half of the sphere, or use its degree 1 and [F5]). Under the wedge isomorphism [F3], a class with coordinates (a,b) is r1a+r2b, since its two restrictions are a,b and the off-diagonal composites are constant. Thus P(a,b)=a+b. For based self-maps f,g, their pinch sum therefore induces (f+g)=f+g. Constant maps induce zero because they factor through the point. By [F5], a degree-d class is the d-fold sum of the identity class; the inverse class has pullback id because its sum with identity is null. Hence every degree-d self-map acts as multiplication by d, for positive, zero and negative d, in every reduced degree.

F3F5algebra
2.1

Apply [F3] to step 1.2. Restriction to the finite wedge summands followed by inverse iterated suspension gives E1p,qαIphq(). A homomorphism from the free cellular chain group is uniquely its values on the oriented cell basis [F4], so this is the required Hom group. Choose each sphere coordinate to match its oriented cell; independence of an orientation-preserving sphere coordinate change follows from [F5], since a degree-one self-map is based homotopic to identity for p1. For vertices use the canonical generator of each singleton; if a negative generator was supplied, negate its coefficient coordinate. Empty cell sets give zero groups on both sides.

F3F4F5step 1.1step 1.2
3.1

Let f:XY be cellular. For p1 its skeletal quotient map is a based map between the sphere wedges of step 1.2. Under [F3], the matrix component from target cell β to source cell α is the pullback of rβfˉια:SpSp, where ι includes a summand and r collapses the others: the insertion of one coefficient is rβ and extraction is ια. By step 1.3 this component is multiplication by the integer degree dβα. The same integers are the cellular chain matrix of f, since those chains are relative homology [F4], and on the sphere quotients the matrix components are the same inclusions and collapses. To compare degree conventions explicitly, in ordinary reduced homology the pinch sends the sphere generator to the pair of generators and the fold adds them; thus a pinch sum acts by the sum of the integers, and identity acts by 1. The classification [F5] therefore makes its integer degree exactly its action on top homology. The Hom pullback is therefore (aβ)β(βdβαaβ)α, exactly the reduced-theory pullback. For p=0, each vertex maps to a vertex and both formulas simply copy its target coordinate; changing chosen vertex signs conjugates both matrices by the same signs. Empty source, empty target when a map exists, and empty cell sets give the zero maps where appropriate.

F3F4F5step 1.2step 1.3step 2.1
4.1

A morphism of reduced theories commutes with maps and suspension by definition [F3]; hence it commutes with summand restriction and the inverse suspension identifications of step 2.1, acting on each coordinate by its homomorphism hq()kq(). Together with step 3.1 this proves both stated naturalities. Above the dimension of X the skeletal quotient is a point and there are no cells. No dimension axiom, restriction on q, or compatibility between separately supplied connecting maps and suspension is needed for this first-page group calculation.

F3step 2.1step 3.1

Source notes

Loizides, §2.1, Remark 2.2 and Lemma 2.3, and the opening of §3 (printed p.4) explain the degree-matrix action and wedge/suspension identification of the first page. The proof here includes negative degrees, empty spaces, the disjoint-basepoint convention at dimension zero, and the negative-degree-map argument explicitly. It uses the cofiber model of relative groups directly and does not invoke a converse reconstruction of all theory structure.

LemmaStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

The AHSS first differential is the cellular coboundary

Statement

Let X be a finite CW complex with chosen cells and orientations, and let h be the CW-pair theory of a reduced generalized cohomology theory. Under the identification E1p,qCcellp(X;hq()) of The AHSS E-one page is cellular cochains with theory coefficients, the first differential of the skeletal exact couple is the cellular coboundary δ:Ccellp(X;hq())Ccellp+1(X;hq()) of the cellular cochain complex with coefficients in the abelian group hq(). Consequently E2p,qHp(X;hq()).

Facts & Assumptions

[F1]

The first page is identified with cellular cochains by E1p,qHom(Cpcell(X),hq()), via the wedge decomposition of Xp/Xp1 and the suspension isomorphisms (The AHSS E-one page is cellular cochains with theory coefficients).

[F2]

In the homological indexing of Exact couple and An exact couple generates a spectral sequence, the initial differential is jk:Ea,b1Ea1,b1 and has bidegree (1,0). Under the cohomological reindexing (p,q)=(a,b) used for the skeletal AHSS, it becomes d1:E1p,qE1p+1,q. Concretely it sends a class on (Xp,Xp1) first by the pair map to hp+q(Xp) and then by the connecting map of (Xp+1,Xp) to hp+q+1(Xp+1,Xp).

[F3]

For p1, a based map SpSp of degree d acts by multiplication by d on any reduced generalized cohomology group of Sp (Degree-d sphere maps act by multiplication by d in any generalized theory).

[F4]

For p1, the incidence number [eτp+1:eσp] is the degree of the attaching-sphere composite onto the σ-sphere. For p=0, an oriented one-cell contributes +1 at its terminal vertex and 1 at its initial vertex (and zero when the endpoints coincide). In every dimension the cellular boundary is the resulting incidence matrix (Incidence number of two CW cells, Cellular boundary is the incidence degree matrix).

[F5]

The cellular cochain complex of the finite CW complex X with coefficients in an abelian group G is the dual of its oriented cellular chain complex (Oriented cellular chain group), so its coboundary has matrix entries [eτp+1:eσp]. Singular cohomology with coefficients in G has choice-free homotopy invariance, pair exactness, excision and the dimension axiom; it also has finite additivity without AC (Singular cohomology satisfies the Eilenberg Steenrod cohomology axioms). Applied to the finite cell decomposition of (Xm,Xm1), excision, finite additivity and the dimension axiom give Hr(Xm,Xm1;G)=0 for rm and identify the group in degree m with the cellular m-cochains. Naturality of the pair connectors identifies the resulting differential with the incidence coboundary.

[F6]

In the associated CW-pair theory, every connecting map is normalized by the fixed suspension as δi=qiσ (Reduced and unreduced generalized cohomology theories correspond). The endpoint and disk orientation calculations are made explicitly below.

[F7]

CW inclusions have the homotopy extension property, and cellular approximation with a finite relative source is choice-free (Relative CW inclusions are cofibrations, Cellular approximation for maps of CW pairs).

Proof

technique · direct

Given: A finite CW complex X with chosen cells and orientations, integers p,q, and the skeletal exact couple whose first page is identified in [F1].

1.1

The differential is d1=jk=jk in the exact-couple indexing: a class in E1p,q=hp+q(Xp,Xp1) is first sent by the pair map k to hp+q(Xp), and then by the connecting map j of the next pair to hp+q+1(Xp+1,Xp)=E1p+1,q.

F2given
1.2

Suppose p1. Restricting along the characteristic map φτ:(Dp+1,Dp+1)(Xp+1,Xp) and collapsing the complement of a p-cell σ exhibits the (τ,σ) component of d1 as the map induced by cσπφτDp+1:SpSp. The disk-boundary connector agrees with positive suspension in these oriented coordinates: cap the oriented disk with the cone on its outward-oriented boundary. The cone has orientation dt followed by the boundary orientation, so its base boundary is the negative of the disk boundary. They glue to an oriented sphere, and collapse of the disk maps the cone to the positively oriented suspension. Thus no extra sign enters the component diagram. To type the characteristic pair map, first approximate its boundary cellularly in Xp, extend that boundary homotopy over the disk by [F7], and approximate the disk rel its now cellular boundary. All sources are finite, and the resulting map is homotopic through pair maps to the original; cellular representatives determine the same maps on the cofiber groups by homotopy invariance. For p1 the boundary vertex now maps into X0Xp1, so the attaching-sphere composite after collapse is based. Its degree is unchanged. This is the attaching map followed by collapse onto the σ-sphere, as in the source diagram.

F1F2F6F7given
1.3

Suppose p=0 and orient a one-cell eτ1 from its initial endpoint v to its terminal endpoint v+. Naturality reduces its component of d1 to the boundary for (D1,S0). The cofiber of (S0)+(D1)+ is a graph consisting of the oriented edge and a spoke from each endpoint to the common cone tip. Its oriented cycle traverses the edge from initial to terminal, then the terminal spoke forwards, then the initial spoke backwards. Collapsing the edge gives the map to Σ(S0)+ with degrees +1 on the terminal circle and 1 on the initial circle. Wedge coordinates, [F3] in dimension one, and the normalized connector [F6] therefore send the endpoint coefficients to a(v+)a(v); hence its coefficient at a vertex v is 1{v+=v}1{v=v}, including zero for a loop.

F2F3F6given
1.4

The cellular coboundary with coefficients hq() has, in the dual cell bases, the incidence entries [eτp+1:eσp] by duality of the cellular boundary.

F4F5
2.1

For p1, the degree action [F3] says that the (τ,σ) component of d1 is multiplication by the degree of the map in step 1.2, namely the incidence number [eτp+1:eσp].

F3F4step 1.2
2.2

For p=0, step 1.3 gives the same incidence coefficient directly, including the negative coefficient at an initial endpoint that cannot be represented by a based self-map of S0.

F4step 1.3
3.1

Steps 2.1 and 2.2 cover all p0 (for p<0 the source is zero, so the differential is zero even when p=1 and the target need not vanish). Their component matrices agree with step 1.4, so d1 is the cellular coboundary under [F1]. The second page is therefore the cohomology of the cellular cochain complex. For completeness, apply the choice-free consecutive-skeleton calculation in [F5]. The pair sequences give Hp(Xp;G)=Cp/imδp1 and identify Hp(Xp+1;G) with the kernel of the induced map to Cp+1; hence this is kerδp/imδp1. Higher cell attachments change neither adjacent group, so finitely many restrictions give Hp(X;G). The same chase starts at X1=, and negative cohomology is zero. Every use of additivity here is over the finite set of cells, so there is no arbitrary family of representative or primitive choices. Taking G=hq() proves the asserted E2 formula.

F1F5step 1.4step 2.1step 2.2
4.1

This proves the stated identification of d1 and the resulting formula for the second page.

step 3.1

Source notes

Compare Loizides, Theorem 3.2 and its component diagram, printed pp. 5–6, where the same matrix computation identifies d1 with the coboundary of cellular cohomology with coefficients hq.

TheoremStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

Cohomological Atiyah–Hirzebruch spectral sequence

Statement

Let X be a finite CW complex, let h~ be a reduced generalized cohomology theory, and let h be the associated CW-pair theory (Reduced and unreduced generalized cohomology theories correspond). There is a cohomological spectral sequence with E1p,q=hp+q(Xp,Xp1),E2p,qHp(X;hq()),dr:Erp,qErp+r,qr+1, whose stable page is the associated graded of the skeletal filtration of Skeletal filtration for generalized cohomology: Ep,qFphp+q(X)/Fp+1hp+q(X). The spectral sequence is natural in X for cellular maps and in the theory h~ for morphisms of reduced generalized cohomology theories.

Facts & Assumptions

[F1]

The pair theory realizes hn(X,A) with a natural long exact sequence and connecting maps, with hn(X)=hn(X,) and hn(X,A)h~n(X/A) for nonempty A (Reduced and unreduced generalized cohomology theories correspond).

[F2]

A page-r homological exact couple consists of bigraded families with maps i:Dp,qDp+1,q1, j:Dp,qEp+1r,q+r1 and k:Ep,qDp1,q exact at all three vertices; an initial exact couple gives a spectral sequence starting at E1=E with differentials of bidegree (r,r1), subquotient description and local-lift formula by An exact couple generates a spectral sequence (Exact couple).

[F3]

The first page is cellular cochains and the first differential is the cellular coboundary, so the second page is Hp(X;hq()) (The AHSS E-one page is cellular cochains with theory coefficients, The AHSS first differential is the cellular coboundary).

[F4]

A cohomological spectral sequence is a homological spectral sequence under Erp,q:=Ep,qr, with differentials of bidegree (r,1r) (Cohomological spectral sequence).

[F5]

The skeletal filtration satisfies Fp+1Fp, Fp=ker(hn(X)hn(Xp1)), Fp+1=ker(hn(X)hn(Xp)), Fp=im(hn(X,Xp1)hn(X)), and it is exhaustive and bounded for finite X (Skeletal filtration for generalized cohomology).

Proof

technique · direct

Given: A finite CW complex X of dimension N, a reduced generalized cohomology theory h~, the associated pair theory h, and the conventions Xp= for p<0, Xp=X for pN.

1.1

Put Dp,q:=hpq1(Xp1) and Ep,q:=hpq(Xp,Xp1), and let i be restriction from Xp1 to Xp2, j the connecting map of the pair (Xp,Xp1), and k the pair map to hpq(Xp). The three exactness conditions are the corresponding portions of the pair long exact sequences: at Dp,q the incoming restriction is hpq1(Xp)hpq1(Xp1) and its image is the kernel of j; the image of j is the kernel of the pair map; and the image of the pair map is the kernel of the outgoing restriction to Xp1. Hence the data form an initial exact couple in the sense of [F2].

F1F2given
1.2

The identification (P,Q)=(p,q) turns the pair (Xp,Xp1) into (XP,XP1) and the group Ep,q=hpq(Xp,Xp1) into hP+Q(XP,XP1); under this reindexing the exact-couple differentials dr:Ep,qEpr,q+r1 become dr:ErP,QErP+r,Qr+1.

F4given
2.1

Applying [F2] to the couple of step 1.1 produces a homological spectral sequence with E1=E, differentials of bidegree (r,r1), subquotients Ep,qrNp,qr/Bp,qr and the local-lift formula ke=ir1xdr[e]=[jx].

F2step 1.1
2.2

The page-1 terms are the cellular cochains and the page-1 differential is the cellular coboundary, so applying the reindexing of step 1.2 to the second page gives E2P,QHP(X;hQ()).

F3step 1.1step 1.2
3.1

By definition of a cohomological spectral sequence, the reindexed data ErP,Q:=EP,Qr form a cohomological spectral sequence whose differentials have bidegree (P,Q)(P+r,Qr+1) and whose second page is HP(X;hQ()), as required.

F4step 2.1step 2.2
3.2

For the convergence, fix (p,q) and put P=p, Q=q, n=P+Q=pq. The numerators Np,qr=k1(im(ir1:Dpr,q+r1Dp1,q)) equal k1(im(hn(XP+r1)hn(XP))), so they decrease with r and stabilize at Np,q=k1(im(hn(X)hn(XP))) once XP+r1=X. The denominators Bp,qr=j(ker(ir1:Dp,qDp+r1,qr+1)) equal j(ker(hn1(XP1)hn1(XPr))), so they increase and, for r>P, equal j(hn1(XP1))=ker(k) because XPr= has zero cohomology.

F1F2F5step 2.1
4.1

The map k sends the stable numerator onto K:=im(hn(X)hn(XP))ker(hn(XP)hn(XP1)) with kernel Bp,q=ker(k), so Ep,q=Np,q/Bp,qK. Restriction hn(X)hn(XP) carries ker(hn(X)hn(XP1)) onto K with kernel ker(hn(X)hn(XP)); hence Ep,qFPhn(X)/FP+1hn(X).

F1F5step 3.2
5.1

The reindexed spectral sequence of step 3.1 has the asserted first and second pages and differentials, and step 4.1 identifies its stable terms with the associated graded of the skeletal filtration. A cellular map preserves every skeleton and therefore gives commuting maps of all the pair sequences used in step 1.1; a morphism of reduced theories gives the same commuting ladders objectwise. These ladders are morphisms of exact couples, so A map of exact couples induces a map of spectral sequences supplies the asserted natural page maps.

step 1.1step 3.1step 4.1

Source notes

Compare Loizides, §3, Theorems 3.2 and 3.4 with Lemma 3.6, printed pp. 4–8, for the exact couple, the E-two page Hp(X;hq) and the identification of E with the associated graded of ker(hn(X)hn(Xm)); and Ji, §§3.1–3.2, printed pp. 10–12, for the right-half-plane support and collapse computations. The indexing here is chosen so that E2p,q=Hp(X;hq()) and dr has bidegree (r,1r).

LemmaStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

Homological AHSS exact couple from the skeletal filtration

Statement

Let X be a finite CW complex with chosen cells and orientations and let h~ be a reduced generalized homology theory. Set Dp,q:=hp+q(Xp),Ep,q:=hp+q(Xp,Xp1), with hn(X,A) the pair groups associated with h~ and the convention Xp= for p<0. Let ip,q:Dp,qDp+1,q1,jp,q:Dp,qEp,q,kp,q:Ep,qDp1,q be induced respectively by the inclusion XpXp+1, by the pair map with respect to (Xp,Xp1), and by the connecting map of that pair. Then (D,E,i,j,k) is an initial exact couple in the sense of Exact couple, its first page is Ep,q1=hp+q(Xp,Xp1)Cpcell(X;hq()), and its first differential d1=jk is the cellular boundary with the incidence-degree matrix. In particular Ep,q2Hp(X;hq()). Here the displayed identification of each sphere summand with hq() is suspension-normalized: it uses the oriented quotient sphere and the structural suspension isomorphisms of the theory. The pair boundary is the cofiber map followed by inverse structural suspension, so the same normalization is used in the calculation of d1.

Facts & Assumptions

[F1]

A reduced generalized homology theory has based homotopy invariance, suspension-compatible cofiber exact sequences, and for a finite wedge an isomorphism αh~n(Sαp)h~n(αSαp) (Reduced generalized homology theory).

[F2]

For a reduced generalized homology theory define the pair groups of a CW pair (X,A) by hn(X,A):=h~n(Ci) for the based inclusion i:A+X+, and hn(X,):=h~n(X+). For A a CW subcomplex inclusion is a based cofibration and the collapse CiX/A is a based homotopy equivalence, so hn(X,A)h~n(X/A). The cofiber exact sequence is the pair long exact sequence, and its natural boundary is the structural cofiber map followed by inverse suspension (Reduced generalized homology theory, Unreduced pair and reduced quotient axioms are equivalent on cw pairs, Relative CW inclusions are cofibrations, Cofiber of a based cofibration is equivalent to the quotient).

[F3]

For p1 the quotient Xp/Xp1 is the finite wedge of the p-spheres belonging to the p-cells, and X0 is a finite discrete set (CW quotients and collapse of a contractible subcomplex, The wedge of a family of pointed spaces).

[F4]

The chosen orientation Dp/Sp1Sp, followed by the p-fold structural suspension isomorphism, gives the canonical coefficient identification h~p+q(Sp)hq() of Coefficient groups of a generalized homology theory. For the disk pair, the pair boundary has target hn1(Sp1)=h~n1((Sp1)+), not merely h~n1(Sp1). Its image is the kernel of hn1(Sp1)hn1(Dp); under the usual based-sphere splitting this kernel is the reduced sphere summand, and [F2] identifies the induced map onto that summand with inverse structural suspension. No isomorphism onto the whole unreduced target is asserted.

[F5]

A based degree-d map SpSp induces multiplication by d on every reduced generalized homology group (Degree-d sphere maps act by multiplication by d in any generalized theory).

[F6]

The cellular p-chains are free on the oriented p-cells, the cellular boundary is the incidence-degree matrix, and cellular homology computes singular homology. The incidence number [eσp:eτp1] is the degree of the composite of the attaching map of eσp with the collapse onto the (p1)-sphere eτp1; the cellular boundary is the incidence-degree matrix (Oriented cellular chain group, Incidence number of two CW cells, Cellular boundary is the incidence degree matrix, Cellular homology computes singular homology).

Proof

technique · direct

Given: A finite CW complex X with chosen cells and orientations, a reduced generalized homology theory h~, and the groups and maps displayed in the statement.

1.1

The exactness conditions of Exact couple hold with r=1: the image of ip1,q+1 equals the kernel of jp,q by exactness of the pair sequence of (Xp,Xp1) at hp+q(Xp); the image of jp,q equals the kernel of kp,q by exactness of that same sequence at Ep,q=hp+q(Xp,Xp1); and the image of kp+1,q equals the kernel of ip,q by exactness of the pair sequence of (Xp+1,Xp) at hp+q(Xp).

F2given
1.2

The wedge decomposition [F3] and the quotient identification of [F2] give Ep,qh~p+q(αIpSαp). The wedge axiom [F1], followed on every oriented sphere summand by the boundary-normalized identification of [F4], gives h~p+q(αIpSαp)αIphq().

F1F2F3F4
1.3

The right-hand side αIphq() is the free cellular chain group Cpcell(X;hq())=αIphq() on the oriented p-cells, and the cellular boundary sends the σ-summand to the sum over (p1)-cells of the incidence numbers.

F6
1.4

The differential is d1=jk. By naturality of the pair boundary for the characteristic map (Dp,Sp1)(Xp,Xp1) and the cofiber-boundary formula in [F2], the σ-summand first maps by the attaching map into hp+q1(Xp1). Projecting with j to the τ-summand composes the attaching map with the collapse Xp1Xp1/Xp2 and then with the projection to the sphere of eτp1. Under the suspension-normalized coordinates of [F4], the resulting coefficient homomorphism is the map induced by that attaching-and-collapse self-map of Sp1; this uses compatibility of the pair boundary with suspension, not an isomorphism from the disk pair group onto all of hp+q1(Sp1).

F2F4given
2.1

For p2, the suspension-normalized comparison in step 1.4 reduces the (τ,σ) component to the self-map of Sp1 defining the incidence number; [F5] therefore makes it multiplication by [eσp:eτp1]. For p=1, the cofiber-boundary convention of [F2] for an oriented characteristic interval gives terminal endpoint minus initial endpoint, so the two possible 0-cell projections have coefficients +1 and 1. For p=0 the target is zero. Thus [F6] identifies d1 with the cellular boundary in every dimension.

F2F4F5F6step 1.4
3.1

Steps 1.1, 1.2 and 2.1 exhibit an initial exact couple whose first page is the cellular chain complex with coefficients hq() and whose first differential is the cellular boundary; hence Ep,q2Hp(X;hq()) by definition of the second page and the identification of cellular with singular homology.

F6step 1.1step 1.2step 2.1
4.1

This proves the asserted exact couple, first page, differential and second page.

step 3.1

Source notes

Compare Davis–Kirk, §8.8 and Theorem 9.6, printed pp. 227–246, for the skeletal exact couple of a generalized homology theory, the identification of the first page with cellular chains and the bidegree of the differential.

TheoremStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

Homological Atiyah–Hirzebruch spectral sequence

Statement

Let X be a finite CW complex and h~ a reduced generalized homology theory. Use the cofiber pair groups hn(B,A)=h~n(CA+B+) and their natural connecting maps, with hn(B)=h~n(B+). Set Xp= for p<0. There is a homological spectral sequence with Ep,q1=hp+q(Xp,Xp1),Ep,q2Hp(X;hq()),dr:Ep,qrEpr,q+r1r, and for each total degree n the filtration Fphn(X):=im(hn(Xp)hn(X)) satisfies Ep,qFphp+q(X)/Fp1hp+q(X). The filtration is finite in each total degree: Fphn(X)=0 for p<0 and Fphn(X)=hn(X) for pdimX when X; for empty X all groups and filtration stages are zero. The second-page isomorphism uses the required suspension-compatible cofiber boundary and boundary-normalized cellular coordinates; there is no independently specified connecting map.

Facts & Assumptions

[F1]

Reduced generalized homology has natural cofiber long exact sequences, homotopy invariance, the wedge axiom, and zero groups on a point; hq()=h~q(S0) and iterated suspension identifies the groups of spheres with these coefficients (Reduced generalized homology theory, Coefficient groups of a generalized homology theory).

[F2]

An initial exact couple generates a spectral sequence starting at E1=E with differentials of bidegree (r,r1) and with the subquotient description Ep,qrNp,qr/Bp,qr, where Np,qr=k1(im(ir1:Dpr,q+r1Dp1,q)) and Bp,qr=j(ker(ir1:Dp,qDp+r1,qr+1)) (An exact couple generates a spectral sequence, Exact couple).

[F3]

A homological spectral sequence has square-zero differentials dr:Ep,qrEpr,q+r1r and specified homology identifications H(Er,dr)Er+1 (Homological spectral sequence).

[F4]

The increasing associated graded consists of the quotients Fp/Fp1 of an already given increasing filtration (Associated graded object of a filtered object).

[F5]

CW subcomplex inclusions are cofibrations, their cofibers are equivalent to their based quotients, and collapsing a nonempty CW subcomplex retains the remaining cells with one quotient vertex (Relative CW inclusions are cofibrations, Cofiber of a based cofibration is equivalent to the quotient, CW quotients and collapse of a contractible subcomplex).

[F6]

Based degree-d maps of positive-dimensional spheres act by d on reduced generalized homology. Cellular boundary coefficients are attaching incidence degrees in dimensions at least two and terminal-minus-initial endpoint coefficients in dimension one; cellular homology computes singular homology (Degree-d sphere maps act by multiplication by d in any generalized theory, Incidence number of two CW cells, Cellular boundary is the incidence degree matrix, Cellular homology computes singular homology).

Proof

technique · direct

Given: The finite CW complex, theory and cofiber pair convention of the statement.

1.1

If X is empty, X+ is a point and every group in question is zero by [F1], proving all assertions in that case. Otherwise put N=dimX. Define Dp,q=hp+q(Xp) and Ep,q=hp+q(Xp,Xp1). Let i be skeletal inclusion, j the pair map and k the pair boundary. The pair exact sequences give imi=kerj, imj=kerk and imk=keri at their respective positions. Their bidegrees are (1,1),(0,0),(1,0), so this is an initial exact couple and [F2] constructs the claimed pages and differentials.

F1F2
1.2

We verify the second page using the suspension-compatible cofiber boundary required by [F1]. Write G=hq(). In column zero, X+0 is a finite wedge of S0's, so E0,q=e0G. For p1, [F5] identifies the skeletal quotient with the finite wedge of oriented p-cell spheres; [F1] initially gives coordinates Ep,q=epG using the specified suspension. For the standard oriented disk pair (Dp,Sp1), its boundary is an isomorphism onto K=ker(hp+q1(Sp1)hp+q1()). Indeed the inclusion of a chosen boundary point makes hm(Sp1)hm(Dp) surjective in every degree, since the disk contracts to that point; the pair exact sequence proves the assertion. For p2, quotienting the chosen boundary point identifies K with h~p+q1(Sp1): the split cofiber sequence S0(Sp1)+(Sp1,s0) proves this, without identifying (Sp1)+ with a based wedge. Use an orientation-preserving identification of the boundary sphere and the specified suspension coordinates to view this disk boundary as an automorphism ap,q:GG. For p=1, K=ker(GG+G) and use the coordinate g(g,g) in initial, terminal order to define the automorphism a1,q.

F1F5
1.3

For fixed (p,q) put n=p+q. Then Np,qr=k1(im(hn1(Xpr)hn1(Xp1))): for r>p the source skeleton is empty, so the image is zero and Np,q=kerk. Likewise Bp,qr=j(ker(hn(Xp)hn(Xp+r1))), and for p+r1N this kernel is ker(hn(Xp)hn(X)).

F1F2
2.1

Naturality for each characteristic disk pair computes jk cell by cell. For p2 its component at a (p1)-cell is the attaching sphere followed by the quotient projection onto that cell. On the reduced kernel just used, this map acts by its degree, by [F6]. This also covers an attaching map that is not based: move its image of one chosen sphere point to the target sphere basepoint along a path and extend that homotopy by the point cofibration [F5]; homotopy invariance gives the same action on the kernel of collapse to a point. Its degree is the incidence number, unchanged by that homotopy. Thus the component is [ep:ep1]ap,q in the initial coordinates. For p=1, naturality sends (a1,qg,a1,qg) to the initial and terminal vertices; when these coincide the sum is zero. The component is again the signed endpoint incidence times a1,q. For p=0 the target is zero. Define T0,q=idG and Tp,q=Tp1,qap,q recursively, and change every coordinate in column p by Tp,q. The new differential component is Tp1,q([ep:ep1]ap,q)Tp,q1=[ep:ep1]idG, since group homomorphisms commute with integer multiplication. Hence the row complex is isomorphic to cellular chains with coefficients G.

F1F5F6step 1.2
3.1

Taking homology of that row gives Ep,q2Hp(X;hq()) by [F3] and [F6]; negative columns are zero. Functoriality of the skeletal inclusions proves FpFp+1 directly. For p<0 the source is zero by [F1], and for pN the map is the identity of hn(X). Thus these images really form a finite exhaustive filtration before [F4] is applied.

F1F3F4F6step 1.1step 2.1
4.1

By exactness, kerk=im(j:Dp,q=hn(Xp)Ep,q). Define Φ:kerkFphn(X)/Fp1hn(X) by choosing xhn(Xp) with j(x)=e and sending e to the image of x in hn(X) modulo Fp1. This is well defined because two such lifts differ by kerj=im(hn(Xp1)hn(Xp)), and it is surjective by the definition of Fp. Its kernel is j(ker(hn(Xp)hn(X))): one inclusion is immediate, and if the image of x lies in Fp1, choose yhn(Xp1) with the same image in hn(X); then xi(y) maps to zero in hn(X) and j(x)=j(xi(y)). Thus step 1.3 gives Ep,q=kerk/j(ker(hn(Xp)hn(X)))Fphn(X)/Fp1hn(X).

F1F2F4step 3.1step 1.3
5.1

Steps 1.1, 3.1 and 4.1 give the asserted first and second pages, the bidegree of the differentials and the identification of the stable page with the associated graded of the finite filtration, which proves the theorem.

step 1.1step 3.1step 4.1

Source notes

The cellular differential and finite convergence construction can also be compared with Duke Lecture 13, proof of Theorem 1.1, pp. 1–3. That source treats spectrum homology. Steps 1.2 and 2.1 above spell out the cellular coordinates under the required suspension-compatible cofiber boundary and keep the orientation choices explicit.

Compare Davis–Kirk, Theorem 9.6, printed pp. 242–243, for the bidegree (r,r1) and the finite skeletal convergence statement, and Miller, Lecture 26, printed pp. 89–92, for the exact-couple filtration conventions.

LemmaStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

Edge maps of a bounded skeletal AHSS

Statement

Let X be a nonempty finite CW complex of dimension N. Consider the skeletal exact couples of given cohomology and homology theories on CW pairs, with natural pair long exact sequences and zero groups on the empty space. Their skeletal spectral sequences have the following edge maps. Set Xp= for p<0 and Xp=X for pN, and put Fphn(X)=ker(hn(X)hn(Xp1)),Fphn(X)=im(hn(Xp)hn(X)). The assertion concerns the spectral sequences of these given pair exact couples; no identification of their second pages is needed.

In cohomology, for every 0pN and every q the pair map k:hp+q(Xp,Xp1)hp+q(Xp) carries a stable cycle of Ep,q to a class in hp+q(Xp) that is the restriction of a class on X, and the induced map Ep,q  Fphp+q(X)/Fp+1hp+q(X),[e][x]where xXp=k(e), is an isomorphism; the lift x is determined modulo Fp+1. In particular the 0-column edge is the quotient hn(X)hn(X)/F1hn(X)E0,n induced by restriction to X0, and the top-column edge EN,nNFNhn(X)hn(X) is the inclusion of the kernel of restriction to XN1.

In homology, the pair map j:hp+q(Xp)hp+q(Xp,Xp1) descends in the opposite direction to an isomorphism Fphp+q(X)/Fp1hp+q(X)  Ep,q, with Fphn(X)=im(hn(Xp)hn(X)). The 0-column edge is the inclusion F0hn(X)=im(hn(X0)hn(X))hn(X), induced by the skeleton inclusion hn(X0)hn(X), and the top-column edge is the quotient hn(X)hn(X)/FN1hn(X)EN,nN.

These identifications require boundedness of the skeletal index only: for each fixed p the stable terms exist because the filtration is finite in p, and no boundedness, vanishing or first-quadrant hypothesis is imposed on the coefficient index q. For empty X, every group and edge map is zero.

Facts & Assumptions

Given: The theories and pair sequences in the Statement. Pair maps and skeletal maps are the usual restriction maps in cohomology and inclusion maps in homology.

[F1]

An initial homological exact couple has i,j,k of degrees (1,1),(0,0),(1,0) and is exact at each vertex (Exact couple).

[F2]

Its spectral pages are Nr/Br, where Nr=k1(imir1) and Br=j(kerir1), with the shifted indices specified in An exact couple generates a spectral sequence.

Proof

technique · direct
1.1

For cohomology use homological indices (a,b), putting Da,b=hab1(Xa1) and Ea,b=hab(Xa,Xa1). The maps i,j,k are respectively restriction, pair boundary and pair-to-absolute map. The given pair sequences prove all three exactness conditions of [F1]. For homology put Dp,q=hp+q(Xp) and Ep,q=hp+q(Xp,Xp1); inclusion, pair map and boundary are i,j,k, and again the pair sequences prove exactness. Thus [F2] applies to both couples. In the cohomological output reindex (a,b)=(p,q).

F1F2given
2.1

Fix 0pN, qZ and n=p+q. Substituting the cohomological groups of step 1.1 in [F2] gives Nr=k1(im(hn(Xp+r1)hn(Xp))) and Br=j(ker(hn1(Xp1)hn1(Xpr))). For rN+2, the former skeleton is X and the latter is empty. Hence N=k1(im(hn(X)hn(Xp))) and B=imj=kerk. Put K=im(hn(X)hn(Xp))ker(hn(Xp)hn(Xp1)). Exactness says imk is the second factor, so k maps N onto K with kernel B. Restriction maps Fphn(X) onto K: a lift x of a member of K restricts to zero on Xp1. Its kernel is Fp+1. The two quotient isomorphisms give exactly the claimed map, with its lift independent modulo Fp+1.

F1F2step 1.1algebra
2.2

In homology [F2] gives Nr=k1(im(hn1(Xpr)hn1(Xp1))) and Br=j(ker(hn(Xp)hn(Xp+r1))). Thus for rN+2, N=kerk=imj and B=j(keru), where u:hn(Xp)hn(X). Define imjFp/Fp1 by j(x)u(x)+Fp1. Two lifts differ by kerj=im(hn(Xp1)hn(Xp)), so this is well defined and surjective. Its kernel equals j(keru): if u(x) comes from yhn(Xp1), subtract the image of y from x to get a lift with zero image in hn(X) and unchanged j(x). Conversely such a lift plainly maps to zero. Quotienting gives Ep,qFp/Fp1. Its inverse is induced by j, not by a map from E1 directly to hn(X).

F1F2step 1.1algebra
3.1

The cohomological filtration has F0=hn(X) and FN+1=0, since restriction to the empty space is zero and restriction to X is the identity. At p=0, step 2.1 identifies the quotient by F1 with the image of restriction to X0 and hence with E0,n. At p=N, its lift x is already a class on X, yielding the inclusion EN,nNFNhn(X). These are precisely the stated cohomological edges.

step 2.1givenalgebra
3.2

Likewise F1=0 and FN=hn(X). At p=0 step 2.2 gives E0,nF0 followed by the inclusion in hn(X); the composite from hn(X0) is the original skeletal inclusion map. At p=N, the map induced by j is the quotient hn(X)hn(X)/FN1EN,nN. Thus the homological edges have the asserted directions.

step 2.2givenalgebra
4.1

The same bound rN+2 worked for every q in steps 2.1 and 2.2. Outside 0pN the pair terms vanish by exactness for an identical pair, so all their later subquotients vanish. No boundedness on q is used. If N=0, the two edges coincide with the identity under the displayed identifications. If X is empty, exactness and the zero absolute groups make all relative groups and pages zero. The representative arguments establish unique cosets and never choose a family of lifts; no additional choice principle is used.

F2step 2.1step 2.2step 3.1step 3.2algebra

Source notes

Loizides, The Atiyah–Hirzebruch Spectral Sequence, §3.2, printed pp.7–8, https://math.gmu.edu/~yloizide/Atiyah-Hirzebruch.pdf , proves the cohomological stable subquotient and its kernel-filtration identification in Lemma 3.6 and Theorem 3.4. Here both variances and the extreme edge maps are calculated directly from the exact-couple subquotient theorem.

TheoremStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

Naturality and edge maps of the AHSS

Statement

Every cellular map f:XY of finite CW complexes induces morphisms of the cohomological and homological Atiyah–Hirzebruch spectral sequences of Cohomological Atiyah–Hirzebruch spectral sequence and Homological Atiyah–Hirzebruch spectral sequence: on every page the induced maps commute with the differentials and the page transitions. A morphism φ:h~k~ of reduced generalized cohomology theories that commutes with suspension and with the cofiber connecting maps induces a morphism of the cohomological spectral sequences; the analogous kind of morphism between reduced generalized homology theories induces a morphism of the homological spectral sequences. These morphisms preserve the edge maps of Edge maps of a bounded skeletal AHSS, and all constructions are compatible with composition and identities.

Facts & Assumptions

[F2]

A morphism of exact couples induces a morphism of their derived couples and of their spectral sequences, preserving every bidegree and page transition, and this construction respects identities and composition (A map of exact couples induces a map of spectral sequences).

[F3]

The two skeletal exact couples are built from the pair long exact sequences of the skeleta and from the suspension and connecting data of the theory (Exact couple, Cohomological Atiyah–Hirzebruch spectral sequence, Homological Atiyah–Hirzebruch spectral sequence).

[F4]

The edge maps are the structural maps of the exact couple under the stable identifications (Edge maps of a bounded skeletal AHSS).

Proof

technique · direct

Given: A cellular map f:XY of finite CW complexes and reduced generalized cohomology and homology theories and their morphisms as above.

1.1

Since f is cellular, it maps Xp into Yp for every p, so on each pair (Xp,Xp1) it induces a map of pairs and hence a map hn(Yp,Yp1)hn(Xp,Xp1) and, in the absolute groups, hn(Yp)hn(Xp). By naturality of the pair long exact sequences and of the suspension isomorphisms these maps commute with i,j,k and define a morphism of the cohomological skeletal exact couples; the homological case is the same with covariant arrows.

F3given
1.2

Identity cellular maps induce identity exact-couple morphisms, and composites of cellular maps induce the composites of the corresponding exact-couple morphisms, by functoriality on every skeletal pair.

F3given
1.3

A morphism φ of reduced generalized cohomology theories commuting with suspension and connecting maps assigns to each pair long exact sequence a commuting ladder, hence defines a morphism of cohomological skeletal exact couples; the same argument for a morphism of reduced generalized homology theories gives a morphism of homological skeletal exact couples.

F3given
2.1

By [F2] the morphisms of step 1.1 and step 1.3 induce morphisms of the derived couples and of every page, commuting with differentials and transitions; composition and identities are respected because the exact-couple construction is functorial.

F2step 1.1step 1.3
3.1

The induced morphisms carry the stable numerator and denominator of the exact couple into the corresponding stable subobjects, so under the edge identifications of [F4] they induce the maps on the filtration stages and filtration quotients; hence the edge maps are preserved.

F2F4step 2.1
4.1

Steps 1.2, 2.1 and 3.1 show that the induced page maps respect identities and composition, commute with all structure, and preserve the edge maps, which proves the theorem in both the cohomological and homological cases.

step 1.2step 2.1step 3.1

Source notes

Compare Davis–Kirk, §9.1, printed pp. 237–246, for naturality of the skeletal exact couple and of its edge maps.

LemmaStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

Pairings of skeletal exact couples induce multiplicative AHSS

Statement

Let h~ be a reduced generalized cohomology theory equipped with a coherent external product: natural bilinear pairings hm(X,A)×hn(Y,B)hm+n(X×Y,A×YX×B) on CW pairs, a unit class in h0(pt), associativity and graded commutativity uv=(1)mnvu for uhm, vhn, compatible with suspension and satisfying the two relative connecting-map Leibniz identities in each variable.

Let X be a finite CW complex with skeleta Xp, let (X×X)n:=i+jnXi×Xj be the skeletal filtration of the product cell structure, and let Δ:XX×X be a cellular approximation of the diagonal, so that Δ(Xs)(X×X)s (Cellular approximation for maps of CW pairs). Write E1p,q=hp+q(Xp,Xp1) for the first page of the cohomological Atiyah–Hirzebruch spectral sequence of Cohomological Atiyah–Hirzebruch spectral sequence and F for the skeletal filtration of Skeletal filtration for generalized cohomology.

(a) The pairing at E1. The relative products of skeletal pairs, the collapse to the (p,r)-summand of the product filtration quotient, and Δ, give for all integers p,q,r,s a bilinear pairing μ1p,q;r,s:E1p,q×E1r,sE1p+r,q+s whose value on xE1p,q=hp+q(Xp,Xp1) and yE1r,s is the composite hp+q(Xp,Xp1)×hr+s(Xr,Xr1)  hp+q+r+s(Xp/Xp1Xr/Xr1)  c hp+q+r+s((X×X)p+r,(X×X)p+r1) Δ hp+q+r+s(Xp+r,Xp+r1), where is the external product and c collapses the summands of (X×X)p+r/(X×X)p+r1 other than Xp/Xp1Xr/Xr1. The same construction pairs the relative groups hm(X,Xp1) and hn(X,Xr1) into hm+n(X,Xp+r1), so the W-terms of the relative skeletal tower are paired with one another as well. The construction is natural in morphisms of theories and under a cellular map g:XY when the chosen filtered diagonals satisfy (g×g)ΔX=ΔYg. No E1 naturality is asserted for arbitrary cellular maps equipped with independently chosen diagonal approximations. From E2 onward the product is the natural cup product. No associativity, graded commutativity or unitality is asserted for μ1, and for a general admitted Δ each of these properties can fail: step 7.2 records an explicit admissible cellular approximation whose first-page pairing is not associative.

(b) Leibniz rule and descent to E2. The pairing of the relative skeletal tower and its cofiber terms is compatible with the tower structure maps and relative connecting maps. Consequently d1(μ1(x,y))=μ1(d1x,y)+(1)p+qμ1(x,d1y)(xE1p,q, yE1r,s). Consequently μ1 carries pairs of d1-cycles to d1-cycles and carries the product of a d1-cycle with a d1-boundary into the d1-boundaries, so it induces a well-defined bilinear pairing μ2p,q;r,s:E2p,q×E2r,sE2p+r,q+s on E2=H(E1,d1).

(c) Bigraded rings from the second page on. The pairing μ2 makes E2 a unital associative graded-commutative bigraded ring, and under the natural isomorphism E2p,qHp(X;hq()) of Cohomological Atiyah–Hirzebruch spectral sequence the product μ2 corresponds to the graded cup product; in particular the E2 product does not depend on the chosen cellular approximation of the diagonal. For every r2 the induced product makes Er a unital associative graded-commutative bigraded ring with dr(μr(x,y))=μr(drx,y)+(1)p+qμr(x,dry)(xErp,q, yErs,t), and Er+1H(Er,dr) is an isomorphism of bigraded rings. The filtration is multiplicative, FpFqFp+q, and the stable product makes EgrFh(X) an isomorphism of graded rings.

Facts & Assumptions

Given: The finite CW complex X with its skeleta, a cellular approximation Δ of the diagonal, and the coherent external product data of the statement: the natural bilinear relative pairings, the unit, associativity, graded commutativity, suspension compatibility and the two relative connecting-map Leibniz identities.

[F1]

The cohomological AHSS of the finite CW complex X has E1p,q=hp+q(Xp,Xp1), differentials dr:Erp,qErp+r,qr+1, second page E2p,qHp(X;hq()), and stable page Ep,qFphp+q(X)/Fp+1hp+q(X), where Fp is the image of hp+q(X,Xp1)hp+q(X) (Cohomological Atiyah–Hirzebruch spectral sequence, Exact couple, Skeletal filtration for generalized cohomology).

[F2]

In the product CW structure the cells are the products of cells of X, with dimensions adding. Hence the n-skeleton is (X×X)n=i+jnXi×Xj and its quotient by the previous skeleton is the wedge i+j=nXi/Xi1Xj/Xj1. A cellular map f:XX×X satisfies f(Xn)(X×X)n for every n, and the cellular-approximation theorem supplies such an approximation Δ of the diagonal, so Δ induces a map of pairs (Xp+r,Xp+r1)((X×X)p+r,(X×X)p+r1) (Cellular approximation for maps of CW pairs).

[F3]

(Cited standard multiplicative structure of a pairing of filtering towers.) Dugger §3.1 uses the relative tower W(A,E)n=F(A/An1,E) and its cofiber terms B(A,E)n=F(An/An1,E), and obtains a pairing of spectral sequences from the compatible pairings (A×B)/(A×B)q+t1A/Aq1B/Bt1,(A×B)q+t/(A×B)q+t1Aq/Aq1Bt/Bt1 built from a multiplication EEE. A pairing of spectral sequences is compatible with every page differential, with the Koszul sign, so on the first page d1 obeys the Leibniz rule. Dugger's Theorem 3.4 proves that in the diagonal case there is a natural isomorphism of rings p,qE2p,q(A,E)p,qHq(A;Epq) with the graded cup product on the right. Miller, MIT 18.906, Lecture 29, printed pp. 100–101, records the corresponding list of properties for a cohomological spectral sequence built from a CW filtration with a chosen skeletal approximation of the diagonal: each Er, is a commutative bigraded algebra, dr(xy)=(drx)y+(1)xx(dry), the isomorphism Er+1H(Er) is one of bigraded algebras, E2,=H(B;H(p1())) as bigraded algebras, FsHnFsHnFs+sHn+n, and EgrH as algebras. Applied to the pairing of the relative skeletal tower and its cofiber terms constructed in steps 1.1–3.1, this standard multiplicative structure gives the first-page Leibniz rule and, for every r2, a unital associative graded-commutative bigraded ring whose differential is a derivation; it also identifies the E2 product with the graded cup product (Dugger, Multiplicative structures on homotopy spectral sequences II, §3.1 with Theorem 3.4, printed pp. 4–5; Miller, MIT 18.906, Lecture 29, printed pp. 100–101).

Proof

technique · direct

Given: A finite CW complex X with its skeleta, a cellular approximation Δ of the diagonal, the skeletal exact couple of [F1], and the coherent external product data of the statement.

1.1

Let xE1p,q=hp+q(Xp,Xp1) and yE1r,s. The external product is a class xy in the cohomology of the quotient Xp/Xp1Xr/Xr1 of the product of pairs (Xp×Xr,Xp1×XrXp×Xr1). By [F2] the quotient (X×X)p+r/(X×X)p+r1 is the wedge of the blocks Xi/Xi1Xj/Xj1 with i+j=p+r, so collapsing every block other than (i,j)=(p,r) defines a map c whose pullback carries a class on that block to a class on the pair ((X×X)p+r,(X×X)p+r1) restricting to the given one on the block.

F2given
2.1

By [F2] the cellular Δ satisfies Δ(Xp+r)(X×X)p+r and Δ(Xp+r1)(X×X)p+r1, so it induces a map of these pairs and Δc(xy)hp+q+r+s(Xp+r,Xp+r1)=E1p+r,q+s; define μ1(x,y) to be this element. Since is bilinear and natural and c and Δ are additive, μ1 is bilinear and natural in morphisms of theories. A cellular map g:XY intertwines the two first-page pairings when its chosen filtered diagonals obey (g×g)ΔX=ΔYg; with independently chosen approximations this square need not commute, so no stronger E1 naturality is claimed.

F1F2step 1.1given
2.2

The same construction with the pairs (X,Xp1) and (X,Xr1) in place of (Xp,Xp1) and (Xr,Xr1) pairs hm(X,Xp1)×hn(X,Xr1) into hm+n(X,Xp+r1). The external product lies in the relative group for (X×X,Xp1×XX×Xr1), and Δ is a map from (X,Xp+r1) to this pair: for zXp+r1 the staircase condition puts Δ(z) in some Xi×Xj with i+jp+r1, hence ip1 or jr1. Write Wpm=hm(X,Xp1) and μW:Wpm×WrnWp+rm+n for these pairings.

F1F2step 1.1given
3.1

The maps Wp+1mWpm induced by the inclusions Xp1Xp, and the maps from the cofiber terms hm(Xp,Xp1) occurring in their long exact sequences, commute with the pairings of steps 2.1 and 2.2 by naturality of the external product and of Δ. The connecting morphisms commute with these pairings by the two relative connecting-map Leibniz identities assumed in the statement. Thus μW and μ1 form the compatible pairing of the relative skeletal tower and its cofiber terms used in [F3].

F2F3step 2.1step 2.2given
3.2

The filtration is multiplicative. Let uFphm(X) and vFrhn(X). By [F1] choose relative lifts u~Wpm and v~Wrn. By step 2.2 the image of μW(u~,v~)Wp+rm+n in hm+n(X) is uv, because both are obtained by pulling the external product back along Δ. Hence uvFp+rhm+n(X).

F1step 2.2given
4.1

By step 3.1 the construction is a pairing of the relative skeletal towers and their cofiber terms. The pairing-of-spectral-sequences result in [F3] therefore applies from the first page, and compatibility with the first differential is precisely d1(μ1(x,y))=μ1(d1x,y)+(1)p+qμ1(x,d1y). The sign uses the total cohomological degree p+q of x, as required by the connecting-map Leibniz identity.

F3step 3.1given
4.2

The stable product is the associated-graded product. For the classes of step 3.2 the image of μW(u~,v~) in the quotient Fp+rhm+n(X)/Fp+r+1hm+n(X) is exactly the class of uv. Under the identification Ep,qFphp+q(X)/Fp+1hp+q(X) of [F1], the pairing of the stable classes is therefore the associated-graded product of h(X).

F1step 3.2
5.1

Consequently μ1 descends to the homology E2=H(E1,d1): if x,y are d1-cycles then step 4.1 gives d1μ1(x,y)=0, so μ1(x,y) is a cycle; if x=d1x and y is a cycle then step 4.1 gives μ1(d1x,y)=d1μ1(x,y), and symmetrically for a boundary in the second variable, so μ1 kills BZ+ZB. A bilinear map vanishing on those subgroups induces a unique bilinear map on Z/BZ/B, which is the asserted pairing μ2 on E2.

F1step 4.1algebra
6.1

The pairing constructed in steps 1.1 to 3.1 is the pairing of the relative skeletal tower and its cofiber terms induced by the external product and Δ, and step 5.1 gives its descent μ2. By [F3], for every r2 the page Er is a unital associative graded-commutative bigraded ring, each dr is a derivation, the comparisons Er+1H(Er,dr) are isomorphisms of bigraded rings, and the E2 product corresponds to the graded cup product under E2p,qHp(X;hq()). Since the latter product is intrinsic and natural in cellular maps, it is independent of the chosen cellular approximation and supplies the asserted natural multiplicative structure from E2 onward.

F1F3step 5.1
7.1

Steps 1.1 to 5.1 establish the first-page pairing of (a) and the Leibniz rule and descent of (b); steps 3.2, 4.2 and 6.1 establish the multiplicative filtration, the associated-graded stable product and the ring structure with derivations from the second page on of (c). All assertions hold for the fixed cellular approximation Δ and, from E2 on, independently of it.

step 5.1step 3.2step 4.2step 6.1
7.2

The restriction in (a) is sharp: the first-page pairing is not associative in general, and the failure is visible in the simplest example. Take X=[0,1] with vertices v0,v1 and oriented edge e, ordinary integral cohomology as h~, and in the square the cellular path (0,0)(0,1)(1,1)(1,0)(0,0)(0,1)(1,1) parameterized linearly on its six segments; the path is cellular and homotopic to the diagonal relative to the endpoints, so it is an admitted Δ, and its image on the oriented edge is Δ[e]=2(v0×e)+2(e×v1)(v1×e)(e×v0). By step 1.1 the extension by zero of the external product is supported on the single block whose two degrees match those of the factors, so for the product of a class in E10,0 with one in E11,0 that block is X0/X1X1/X0, whose cells are v0×e and v1×e: the terms 2(v0×e) and (v1×e) of Δ[e] contribute, and the term (e×v0) does not. Hence the class a with a(v0)=1, a(v1)=0 and the class z with z(e)=1 satisfy μ1(a,a)=a and μ1(a,z)=2z by step 2.1, so μ1(μ1(a,a),z)=2z4z=μ1(a,μ1(a,z)) in E11,0Z. The first page therefore carries the pairing and Leibniz structure of (a) and (b) but is not a ring for this admissible Δ. The failure does not descend to E2: here the first differential is the cellular coboundary, so z is a d1-boundary and a is not a d1-cycle, while d1z=0 because E12,0=h2(X,X)=0; hence z and μ1(a,z)=2z vanish in E2, E21,0=H1(X;Z)=0, and by step 6.1 the induced product on E2 is still the cup product.

givenstep 1.1step 2.1step 5.1step 6.1
8.1

Steps 1.1 to 7.2 prove, for a finite CW complex and a cellular approximation of the diagonal, the typed first-page pairing with its Leibniz rule, its descent to E2, and the bigraded ring structure with derivations from the second page on, together with the multiplicative filtration and the associated-graded stable product; they also record that the first page itself is not a ring in general.

step 7.1step 7.2

Source notes

Compare Dugger, Multiplicative structures on homotopy spectral sequences II, §2.2, §3.1 and §3.3 with Theorem 3.4, printed pp. 2–5. His §3.1 pairs the filtering towers by the maps (A×B)/(A×B)q+t1A/Aq1B/Bt1 and (A×B)q+t/(A×B)q+t1Aq/Aq1Bt/Bt1; the proof of Theorem 3.4 computes the pairing on the first page and finds that it differs from the product of coefficient-ring values by the Koszul sign (1)sq, the sign already used in defining the graded cup product of §2.2; and in the diagonal case, where he needs only a map Δ homotopic to the diagonal that preserves the cellular filtration, the theorem itself states "there is a natural isomorphism of rings p,qE2p,q(A,E)p,qHq(A;Epq)", the right-hand side being the graded cup product. That is the identification used in [F3] and in step 6.1, and the first-page pairing compared in that proof, up to the Koszul sign, is the one reconstructed in steps 1.1–3.1, including the extension by zero on the individual blocks of the quotient by the previous product skeleton.

Compare Miller, Lecture 29, printed pp. 100–101, for the list of properties carried by the pages from the second page on: each Er, is a commutative bigraded algebra, dr(xy)=(drx)y+(1)xx(dry), Er+1H(Er) as bigraded algebras, E2,=H(B;H(p1())) as bigraded algebras, FsHnFsHnFs+sHn+n and EgrH as algebras. Miller states this list for the cohomological spectral sequence of a fibration, says that its construction from a CW filtration "requires us to choose a skeletal approximation of the diagonal", and then declines to justify the multiplicative behaviour further. Dugger's theorem is stated for the homotopy spectral sequence of a ring spectrum and Miller's list for the cohomological case; neither states the multiplicative structure of the cohomological AHSS of an abstract generalized cohomology theory with external-product data verbatim. That is why this item proves the first-page pairing, its Leibniz rule and its descent to E2 directly from the stated hypotheses, and cites the standard multiplicative structure of a pairing of filtering towers, the common content of both sources, only for the ring structure of the pages from E2 on.

The failure recorded in step 7.2 is the reason the earlier form of this item, which asserted a bigraded ring on every page including E1, cannot be kept. It also shows why independently chosen filtered diagonals do not give a natural first-page product: homotopic diagonal approximations can induce different block multiplicities on E1. On the interval the six-segment path traces the boundary square once and then the left and top edges from (0,0) to (1,1), so it is homotopic to the diagonal relative to the endpoints; the multiplicity 2 on the block {v0,v1}×e is not homotopy invariant there, and the class z that exhibits the failure does not survive to E2: the first differential is the cellular coboundary, so z is a d1-boundary and E21,0=H1(X;Z)=0. The pages from E2 on are therefore unaffected, which is exactly the sense in which diagonal homotopies act trivially from the second page on. Compare Ji, §1.3, printed p. 4, where it is stated that as given the Atiyah–Hirzebruch spectral sequence gives no information about the multiplicative structure of a generalized cohomology theory: a first-page ring is not available in the literature and is not asserted here.

TheoremStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

Multiplicative AHSS for a multiplicative generalized theory

Statement

Let h~ be a reduced generalized cohomology theory with a specified unital, associative, graded-commutative coherent external product compatible with suspension and satisfying the two relative cofiber-boundary Leibniz identities. Then for a finite CW complex X and a cellular approximation Δ:XX×X of the diagonal the cohomological AHSS of Cohomological Atiyah–Hirzebruch spectral sequence is multiplicative from its second page on: the relative products of skeletal pairs and Δ pair the skeletal exact couple with itself, that pairing is a Leibniz pairing for d1 and descends to E2, and for every r2 the page Er is a unital associative graded-commutative bigraded ring on which dr is a derivation of total degree one, dr(xy)=dr(x)y+(1)p+qxdr(y)(xErp,q), with Er+1H(Er,dr) an isomorphism of bigraded rings. The product on E2 corresponds to the graded cup product under the natural isomorphism E2p,qHp(X;hq()), so it is independent of the chosen cellular approximation of the diagonal. The skeletal filtration is multiplicative, FpFqFp+q, and EgrFh(X) as graded rings. The first page carries the pairing and its Leibniz rule but is not a ring in general: Pairings of skeletal exact couples induce multiplicative AHSS records an admissible cellular approximation whose first-page pairing is not associative. A ring prespectrum is one source of such external-product data, not a hypothesis imposed by the theorem: any data satisfying the displayed properties qualify.

Facts & Assumptions

[A1]

The external product data assumed in the statement comprise the natural bilinear relative pairings, the unit, associativity, graded commutativity, suspension compatibility and the two Leibniz identities (Pairings of skeletal exact couples induce multiplicative AHSS).

[A2]

The finite-CW cohomological AHSS has the skeletal exact couple of Cohomological Atiyah–Hirzebruch spectral sequence, and its stable page is the associated graded of the skeletal filtration.

[A3]

The skeletal exact couple paired with itself through Δ carries the typed first-page pairing of the pairing lemma, a Leibniz rule for d1, the descent of the pairing to E2; from E2 on the page products make each page a unital associative graded-commutative bigraded ring on which the differential is a derivation, with Er+1H(Er,dr) as rings; the product on E2 is the graded cup product under E2p,qHp(X;hq()), so homotopic cellular approximations of the diagonal agree from the second page on and the first page is not in general a ring; the filtration is multiplicative and the stable product is the associated-graded product (Pairings of skeletal exact couples induce multiplicative AHSS).

Proof

technique · direct

Given: A reduced generalized cohomology theory h~ with the external product data of [A1], a finite CW complex X, and a cellular approximation Δ of the diagonal.

1.1

The assumed data satisfy exactly the hypotheses of the pairing lemma [A3]: the relative products are natural and bilinear, the unit, associativity and graded-commutativity hold, the two relative boundary Leibniz identities are assumed, and Δ is a cellular approximation of the diagonal of the finite complex.

A1given
1.2

The skeletal exact couple, its first page, its second page and its stable identification are those of [A2], so the pairing lemma applies to this couple and to this diagonal approximation.

A2given
2.1

Applying [A3] gives the typed first-page pairing, its Leibniz rule for d1 and its descent to E2; from the second page on it gives the ring products, the derivation identity dr(xy)=dr(x)y+(1)p+qxdr(y) for r2, the ring comparison Er+1H(Er,dr) and the identification of the E2 product with the graded cup product, hence its independence from the chosen cellular diagonal from E2 onward; and it gives the inclusion FpFqFp+q together with the identification of E with the associated graded.

A3step 1.1step 1.2
3.1

Step 2.1 is exactly the asserted multiplicative structure from the second page on, together with the first-page pairing and its Leibniz rule and the exclusion of a general first-page ring; no representability or ring-spectrum hypothesis is used, since only the listed product data and the pairing lemma's construction enter.

step 2.1

Source notes

Compare Miller, Lecture 29, printed pp. 100–101, for the product structure on each page from the second page on, the derivation property and the associated-graded ring statement in the ordinary-cohomology case; and Dugger, Multiplicative structures on homotopy spectral sequences II, §3.1 with Theorem 3.4, printed pp. 4–5, for the pairing of filtering towers and the identification of the second-page product with the graded cup product on which the independence from the diagonal approximation rests.

PropositionStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

AHSS collapse generally determines only the associated graded object

Statement

For a convergent Atiyah–Hirzebruch spectral sequence on a finite CW complex, equipped with its finite skeletal abutment filtration, collapse determines the associated graded family of the abutment: the quotients Fphn(X)/Fp+1hn(X) in cohomology or Fphn(X)/Fp1hn(X) in homology. These are the data supplied by convergence. Reconstructing the filtered abutment from these data is the extension problem; collapse alone supplies no splitting. Multiple nonzero quotients may leave additive extensions to resolve and, for a multiplicative spectral sequence, multiplicative extensions. A one-jump filtration has no additive extension problem. Thus there is no general reconstruction rule based solely on collapsed-page and associated-graded data. The algebraic examples below demonstrate this limitation of those data; they do not assert that each displayed filtered object is realized by an AHSS.

Facts & Assumptions

[F1]

Abutment data identify stable-page entries with the successive quotients of a finite, exhaustive, separated filtration in each total degree; in decreasing cohomological indexing the quotient is Fp/Fp+1 (Abutment to a filtered object).

[F2]

The extension problem consists of reconstructing an object from its associated graded pieces through the short exact sequences 0Fp+1Fpgrp0; specifying the outside objects does not specify the middle one or the maps, and a splitting is extra data (Extension problem of a convergent spectral sequence, Associated graded object of a filtered object).

[F3]

A filtration of an abelian group determines the associated graded as the indexed family of its successive quotients; no converse reconstruction of the group is asserted (Associated graded object of a filtered object).

Proof

technique · direct

Given: A convergent AHSS with the stated finite abutment filtration and a collapsed page E2=E.

1.1

By [F1] the collapsed page determines exactly the filtration quotients Fp/Fp+1 (cohomologically) or Fp/Fp1 (homologically); nothing in the identification uses or supplies the extension classes, and the collapse hypothesis only asserts the vanishing of the differentials, so it adds no data beyond the pages.

F1F2given
1.2

Additively, let A=Z/4 with the filtration F0=A, F1=2Z/4Z/2, F2=0, and let B=Z/2Z/2 with the filtration F0=B, F1=0Z/2, F2=0. Both graded families have Z/2 in degrees zero and one and zero elsewhere. (They can also be packaged as a finite direct sum, but that packaging is not the definition.) Yet A has an element of order four and every element of B is killed by two, so they are not isomorphic; hence the additive extension data are not determined by the graded pieces.

F2F3given
1.3

Multiplicatively, an ambiguity can remain even when the additive groups are known. Set A=F2[x]/(x4) and R=F2[u,v]/(u2,v2). Give A the filtration F0=A, F1=(x2), F2=0 and R the filtration F0=R, F1=(v), F2=0, extending by the whole ring below zero and zero above one. Both are multiplicative since the displayed ideals square to zero. In each case the degree-zero quotient is F2[a]/(a2) and the degree-one piece is its free rank-one module generated by z; products of two degree-one pieces vanish. Thus their graded rings are both F2[a,z]/(a2,z2) with filtration degrees a=0, z=1. Their additive groups are both F24, as witnessed by bases 1,x,x2,x3 and 1,u,v,uv. But xA is nilpotent with x20, whereas every nilpotent of R has constant coefficient zero and squares to zero. The rings cannot be isomorphic. These are explicitly computed filtered rings, not claimed AHSS realizations.

F2F3algebra
1.4

If the sole nonzero quotient of a finite decreasing filtration is Fj/Fj+1, all earlier quotients zero force equality of the preceding stages with the whole group, and all later quotients zero force equality of the following stages with zero. Hence Fj=H, Fj+1=0 and that quotient is H itself. If every quotient vanishes, finite exhaustiveness and separation similarly force H=0. Reversing indices gives the increasing case. Multiple quotients do not force ambiguity in every example; they merely permit an extension problem.

F1F2F3algebra
2.1

Steps 1.1 to 1.3 show that the collapsed pages determine the associated graded object and that distinct filtered objects, additively and multiplicatively, share that associated graded; so the pages alone do not contain general extension data. Step 1.4 records the zero and one-jump exceptions. This establishes the stated limitation without claiming that every individual collapse is ambiguous.

step 1.1step 1.2step 1.3step 1.4

Source notes

Compare Davis–Kirk, §9.1, printed pp. 237–246, for the associated graded filtration of the abutment and the resulting extension problem, and Sharifi, §4.1, printed pp. 87–90, for the extension problem.

CorollaryStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

Complex K-theory AHSS

Statement

Assume AC. For a finite CW complex X the Atiyah–Hirzebruch spectral sequence of complex topological K-theory has E2p,q{Hp(X;Z),q even,0,q odd,dr:Erp,qErp+r,qr+1, and converges to the associated graded of the skeletal filtration of qKp+q(X); equivalently Ep,qFpKp+q(X)/Fp+1Kp+q(X). The assumption AC is inherited from the construction of complex K-theory and its coefficients, not from the spectral-sequence machinery.

Facts & Assumptions

[A1]

Assume AC. On finite CW pairs the groups Kq form a contravariant two-periodic multiplicative generalized cohomology theory with coefficients K2k()Z and K2k+1()=0 (Complex K-theory is a two-periodic generalized cohomology theory).

[A2]

Bott periodicity gives the natural isomorphisms Kq(X)Kq2(X) used to read the coefficient groups in every degree (Complex Bott periodicity).

[A3]

The cohomological AHSS of a reduced generalized cohomology theory on a finite CW complex has E2p,q=Hp(X;hq()), differentials of bidegree (r,1r) and stable page the associated graded of the skeletal filtration (Cohomological Atiyah–Hirzebruch spectral sequence).

Proof

technique · direct

Given: Assume AC and let X be a finite CW complex.

1.1

The reduced groups K~q constructed in [A1] on based finite CW complexes satisfy the reduced generalized-cohomology axioms, and the absolute and relative groups Kq in [A1] are the associated pair theory. Thus [A3] applies to K~ and abuts to the stated skeletal filtration of Kq(X). Its coefficient groups are K2k()Z and K2k+1()=0 by [A1], and [A2] supplies the two-periodic identifications in every integer degree.

A1A2A3given
2.1

Substituting hq()=Kq() into E2p,q=Hp(X;hq()) gives E2p,q=Hp(X;Z) for even q and E2p,q=0 for odd q, while the differential bidegree and the convergence statement are those of [A3].

A3step 1.1
3.1

Steps 1.1 and 2.1 give the displayed second page, the differential bidegree and the identification of the stable page with the associated graded of the skeletal filtration; the Axiom of Choice enters only through the inherited complex K-theory construction.

step 1.1step 2.1

Source notes

Compare Ji, §3.1, printed pp. 10–11, where the parity of the coefficient groups is used to read the K-theory AHSS.

LemmaStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

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.

LemmaStatement: Literature-sourcedProof: AI-generatedaudited 2026-09-22Open item page →

KU representability and the skeletal–Postnikov d-three comparison

Statement

Assume AC. On finite CW pairs the Bott-compatible Ω-prespectrum KU of May represents the locally defined complex topological K-groups K constructed from vector bundles: there are natural isomorphisms KUn(X,A)Kn(X,A) for all n, compatible with suspension and the cofiber connecting maps. After Bott translation of any coefficient row to coefficient index at most 2, Adams's connective cover kuKU identifies the E3 source, the E3 target and the differential d3 of the two skeletal Atiyah–Hirzebruch spectral sequences in that row. At bidegree (p,q), put t=p+q. For p1 the resulting skeletal d3 on a class represented by a cellular E1-cocycle is exactly the cellular lifting obstruction given by the Postnikov invariant of the total-degree representing space kut linking πp(kut)=πq(ku) to πp+2(kut)=π2q(ku). Under the stable Bott identifications this is the corresponding translate of the first stable ku invariant. It is independent of the chosen lifts; the case of a finite CW pair follows by passing to the quotient.

Facts & Assumptions

[A1]

Assume AC. For a finite CW complex Y one has [Y,Z×BU]K~0(Y): the finite-rank complement theorem writes virtual bundles as [E][εN], stable classification identifies them with component ranks of classifying maps, and the common-summand relation proves the identification in both directions (Finite-rank complement theorem over compact Hausdorff bases, Real and complex vector bundles are classified by stable Grassmannians, Complex topological K⁰ by Grothendieck completion).

[A2]

Assume AC. KU denotes May's Bott-compatible Ω-prespectrum with KU2i=Z×BU and KU2i+1=U, whose adjoint structure maps are the loop and Bott equivalences; the associated cohomology theory has KUn(X,A)Kn(X,A), with all naturalities. Complex K-theory is the two-periodic generalized cohomology theory of Complex K-theory is a two-periodic generalized cohomology theory with the Bott isomorphisms of Complex Bott periodicity (Sequential prespectra, spectra, and adjoint structure maps, Stable homotopy groups of a sequential prespectrum).

[A3]

Assume AC. Adams's connective cover kuKU has πk(ku)=0 for k<0 and maps isomorphically onto πk(KU) for k0; as a spectrum it represents a reduced generalized cohomology theory on based finite CW complexes, and the spectrum map induces a morphism of reduced theories. Its first k-invariant is the stable operation δ2Sq2 (Sequential prespectra, spectra, and adjoint structure maps, Stable homotopy groups of a sequential prespectrum, The first connective complex K-theory Postnikov invariant is integral Sq-three; Adams Chapter 6(v), printed pp. 245–246).

[A4]

The cohomological AHSS of a finite CW complex has E1p,q=hp+q(Xp,Xp1), d1 the cellular coboundary and E2p,q=Hp(X;hq()), and the exact-couple machinery gives, for every r and every class e with k(e)=ir1x in the skeletal couple, dr[e]=[j(x)] with j the connecting and k the pair map (Cohomological Atiyah–Hirzebruch spectral sequence, The AHSS E-one page is cellular cochains with theory coefficients, An exact couple generates a spectral sequence).

[A5]

Assume AC. For a represented extraordinary cohomology theory, Maunder's comparison theorem identifies, from E2 onward and compatibly with every differential, the spectral sequence from the skeletal filtration of the source with the spectral sequence from the Postnikov tower of the representing spaces. At bidegree (p,q) of total degree t=p+q, the relevant representing space is kut, because πp(kut)=πpt(ku)=πq(ku) (Maunder, Theorem 3.3). The Postnikov invariant joining this group to πp+2(kut) is the primary obstruction of the relevant Postnikov fibration, and cellular lifting obstruction theory evaluates it on attaching maps independently of the chosen partial lifts (Postnikov k-invariant, Obstruction theory for lifting through a fibration, Eilenberg--Mac Lane spaces represent singular cohomology). The comparison is applied componentwise to this representing space, not to the spectrum as though it were a single space.

Proof

technique · direct

Given: Assume AC, finite CW pairs, the bundle model K, May's prespectrum KU and Adams's connective cover ku.

1.1

For a based finite CW complex Y the finite-rank complement theorem and stable classification identify K~0(Y) with the based homotopy set [Y,Z×BU]: every virtual class has the form [E][εN]; adding trivial summands does not change the stabilized classifying map; and a homotopy of classifying maps gives the corresponding stable bundle isomorphism. The common-summand relation therefore identifies both directions naturally.

A1given
1.2

The adjoint structure maps of KU are equivalences, so KU represents a cohomology theory; the degree-zero bundle-classification identification, the suspension adjunction and the natural Bott maps identify KUn(X,A) with the two-periodic Kn(X,A) in every degree, because both connecting maps are induced by the same quotient map followed by suspension.

A1A2given
1.3

If the chosen KU coefficient row is odd, its source and target groups are zero and the comparison assertion is vacuous. Thus fix p1 on a nonzero row and Bott-translate it to an even index q2. Put t=p+q. A bidegree-(p,q) class has total cohomological degree t, so its representing space in Maunder's comparison is kut, not kuq. The spectrum-space indexing gives πp(kut)=πpt(ku)=πq(ku)Z, πp+1(kut)=π1q(ku)=0,πp+2(kut)=π2q(ku)Z. Apply [A5] to the component containing the representing map. It gives an isomorphism from E2 onward between the skeletal AHSS of [A4] and the Postnikov spectral sequence for kut, commuting with d3.

A3A4A5given
2.1

In the Postnikov spectral sequence of step 1.3, the vanishing of πp+1(kut) makes the first possible differential out of this bidegree the operation represented by the relevant class kp+3 linking πp(kut) to πp+2(kut). This need not be the first Postnikov invariant of the whole space kut: by [A3] it is the Bott translate, in this coefficient row, of the first stable ku invariant. By the definition and lifting theorem cited in [A5], evaluating it on a cellular cocycle is the primary obstruction to lifting the corresponding map through that Postnikov stage: on each oriented (p+3)-cell it is obtained from the attaching map, and changing the partial lift changes the obstruction cochain by a coboundary. Maunder's differential-compatible comparison transports exactly this obstruction class to the skeletal d3.

A3A5step 1.3
2.2

Bott-translate any coefficient row to q2. Since Eq()=πq(E) for a representing spectrum, kuKU is an isomorphism on the coefficient groups in the source row q and target row q2. It is also an isomorphism on the intervening odd rows, both of which are zero. Hence its map of skeletal exact couples induces isomorphisms on the relevant E2 and E3 source and target groups and commutes with d3.

A3A4step 1.2
3.1

Maunder's comparison and the relevant Postnikov obstruction in step 2.1 apply componentwise for every p1, including p=1; no class in Hp is evaluated on a space indexed by q. For a finite CW pair (X,A), apply the reduced comparison to the finite quotient X/A; represented cohomology identifies this with the relative group and preserves the skeletal filtration and connecting maps.

A2A5step 2.1given
4.1

Combining steps 1.3, 2.1 and 2.2 identifies the skeletal d3 of the K-AHSS with the relevant Postnikov obstruction in the total-degree space kup+q, equivalently the coefficient-row translate of the first stable ku invariant. Step 1.2 identifies the local K-groups with those represented by KU, and step 3.1 covers all p1 and finite CW pairs.

step 1.2step 1.3step 2.1step 2.2step 3.1
5.1

Steps 1.2 and 4.1 give the asserted representability, the E3 comparison in nonpositive coefficient rows and the identification of the skeletal d3 with the Postnikov obstruction.

step 1.2step 4.1

Source notes

The representability statements are May's Chapter 22 §2 and Chapter 24 §§1–2, printed pp. 175–179 and 204–208; the connective cover and its stable homotopy are Adams's Chapter 2 and Chapter 6(v), printed pp. 174–179 and 245–246, with the first k-invariant supplied by Proposition 16.6 at pp. 391–393. The comparison between the skeletal and representing-space Postnikov spectral sequences is Maunder's Theorem 3.3; it supplies isomorphisms from E2 onward commuting with every differential. Adams identifies the ku invariant, while Maunder is the missing comparison that makes it the skeletal d3.

TheoremStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

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.

5 · Examples, counterexamples and false statements

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