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Finite additivity alone does not prove infinite cw uniqueness

Statement refuted

Finite additivity cannot replace arbitrary additivity in uniqueness on all CW pairs. For every integer n, set En(X)=(i0H~i(X;Z))/(i0H~i(X;Z)). This construction on based CW spaces satisfies the reduced homotopy, exactness, excision, suspension, and dimension axioms with zero coefficient group, and finite wedge additivity, but fails arbitrary wedge additivity. Its pair version is En(X,A)=(i0Hi(X,A;Z))/(i0Hi(X,A;Z)). The theory Hn(X,A;Z)En(X,A) satisfies the unreduced ordinary axioms with coefficient Z except arbitrary additivity, agrees with H on every finite-dimensional CW pair, and differs on W=i1Si.

Facts & Assumptions

Given: The objects and hypotheses in the statement above.

[F1]

Ordinary unreduced theories on CW pairs and reduced ordinary theories on based CW spaces with vertex basepoints determine one another, naturally and compatibly with morphisms and coefficients. For A the correspondence gives hn(X,A)h~n(X/A); for A= it gives hn(X)h~n(X+), where X+=X{}. Under this correspondence, pair boundaries are cofiber boundaries followed by inverse suspension, and arbitrary disjoint-sum additivity corresponds to arbitrary wedge additivity. For a CW triple BAX there is a natural exact sequence hn(A,B)hn(X,B)hn(X,A)hn1(A,B), whose last map is the pair boundary followed by hn1(A)hn1(A,B). (Unreduced pair and reduced quotient axioms are equivalent on cw pairs)

[F2]

For any abelian group G, H0(;G)G and Hn(;G)=0 for every integer n0. For every set-indexed family of pairs the canonical map αHn(Xα,Aα;G)Hn(αXα,αAα;G) is an isomorphism. Together with the structural axioms, singular homology is an ordinary theory with coefficient group G. (Singular homology satisfies dimension and arbitrary additivity)

[F3]

For a CW pair (X,A), an ordinary theory h with coefficient G, and chosen cell orientations, the complex Ch(X,A) is canonically Ccell(X,A;Z)G. Its differential is the integral incidence matrix acting on G. In degree one the entries are signed terminal-minus-initial endpoints. The direct-sum matrices have finite support in each column. (Axiomatic cellular boundaries are integral incidence matrices with coefficients)

[F4]

For every finite-dimensional CW pair (X,A) and ordinary theory h, there is a canonical isomorphism hn(X,A)Hn(Ch(X,A)) for every integer n, natural for cellular maps. It is the skeletal lift isomorphism described below and commutes with the homology connecting maps of pairs. The number of cells need not be finite. (Finite dimensional skeletal exactness computes axiomatic homology)

[F5]

For every ordinary theory h with arbitrary additivity and every CW pair (X,A), the canonical map colimi0hn(Xi,Ai)hn(X,A) is an isomorphism. So is the canonical colimit over finite subcomplex pairs (K,KA) of X. The latter identification is natural for every continuous map of CW pairs. (Additivity and compact cell support control the infinite cw colimit)

Counterexample

1.1

For a family of abelian groups Mi, denote i0Mi/i0Mi by Q(M). Degreewise maps induce maps of Q, giving functoriality. If AiuiBiviCi is exact at every Bi, then Q(A)Q(B)Q(C) is exact: when v(b) is finitely supported, replace the finitely many bad coordinates of b by zero; the resulting equivalent tuple lies in kervi. Choose coordinate lifts in Ai and obtain a preimage in Q(A). The converse inclusion follows from viui=0. This uses ordinary choice for the countable family of nonempty lift sets. Adding, deleting, or altering finitely many initial coordinates has no effect on Q.

constructalgebra
2.1

Apply step 1.1 to the ordinary singular pair sequence supplied by [F2]. Define the E boundary by sending a representative (xi)i0 to the tuple whose jth coordinate is the singular boundary xj+1Hj(A;Z). Dropping the unused initial coordinate is precisely the shift identification of step 1.1. At each term the coordinatewise singular exact sequence and that shift prove the required exactness, even though En is independent of nZ. Homotopies and excision induce coordinatewise equal maps and isomorphisms, so they do so on Q. Apply [F1] here only to the ordinary singular theory [F2]: its quotient identifications and suspension isomorphisms give coordinatewise reduced cofiber sequences and suspension maps. Applying Q and step 1.1 gives the reduced E axioms and identifies them with the displayed pair construction. Replacing reduced absolute groups by unreduced absolute groups changes only coordinate zero and therefore does not change Q. All structure maps are natural.

F1F2step 1.1construct
2.2

A point, the empty space under the zero reduced-empty convention, and S0 have reduced homology in at most one degree. Their Q groups vanish; hence the coefficient of E is zero. For any finite family, the product over degrees commutes with its finite direct sum, as does the finite-support subgroup. Thus finite disjoint-sum additivity holds for pairs and finite wedge additivity for reduced spaces. For a finite-dimensional CW pair of dimension at most N, [F3] and [F4] applied to singular homology give Hi(X,A;Z)=0 outside 0iN, regardless of the number of cells. Therefore En(X,A)=0 for every integer n.

F2F3F4step 1.1algebra
3.1

Give W=i1Si its CW structure with one vertex and one cell in each positive dimension, all attached by constant maps. The cellular differentials vanish, including the degree-one terminal-minus-initial differential. On each skeleton [F3] and [F4] compute one copy of Z in each positive degree present. Applying [F5] to ordinary singular homology, not to E, gives H~i(W;Z)=Z for every i1 and zero in degree zero. Hence En(W)=i1Z/i1Z0: the all-ones tuple is not finitely supported. Yet each En(Si)=0 by step 2.2, so the canonical infinite wedge map from the direct sum of these zero groups is not surjective.

F3F4F5step 2.2algebra
4.1

Taking the direct sum of the pair functors H and E, with componentwise structure maps, preserves homotopy, exactness, excision, dimension, and finite additivity. Its coefficient at a point is Z0=Z, and step 2.2 identifies it with H on all finite-dimensional pairs. On W, ordinary H1(W;Z)=0 by the nonnegative singular chain complex, whereas (HE)1(W)=E1(W)0 by step 3.1. Thus even an abstract graded-group equivalence fails there. The ordinary all-CW uniqueness theorem requires arbitrary additivity, exactly the axiom that this construction fails.

F2step 2.1step 2.2step 3.1algebra

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