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LemmaStatement: Literature-sourcedProof: AI-adaptedPipeline-generatedjudge pass (gpt-5.6-terra)audited 2026-09-07
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  • Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
  • AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
  • AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.

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Any ordinary homology theory has a cellular chain complex on a cw pair

Statement

For a CW pair (X,A) and an ordinary theory h with coefficient G, put F−1=A and Fr=A∪Xr for r≥0. Set Crh(X,A)=hr(Fr,Fr−1)(r≥0),Crh=0(r<0). Each Crh is the direct sum of copies of G indexed by the relative r-cells. Define d0=0 and for r≥1 let dr be the triple boundary to hr−1(Fr−1,A) followed by its map to hr−1(Fr−1,Fr−2). Then dr−1dr=0, naturally for cellular maps of CW pairs.

Facts & Assumptions

Given: The objects and hypotheses in the statement above.

[F1]

Let h be an ordinary theory with coefficient group G=h0(∗). For every n≥0 and k∈Z, hk(Dn,Sn−1)≅{Gk=n,0k≠n. At n=0 the pair means (∗,∅). Also h~k(Sn)≅G for k=n and zero otherwise, including n=0. Choose the disk identifications by ordered orientations and iterated cone boundaries, so they commute with these boundaries. (Any ordinary homology theory computes relative cell groups from its coefficient group)

[F2]

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 B⊂A⊂X there is a natural exact sequence ⋯→hn(A,B)→hn(X,B)→hn(X,A)→hn−1(A,B)→⋯, whose last map is the pair boundary followed by hn−1(A)→hn−1(A,B). (Unreduced pair and reduced quotient axioms are equivalent on cw pairs)

[F3]

Write Xn for the union of cells of dimension at most n, with X−1=∅. A CW subcomplex A⊆X is a union of open cells such that, whenever A contains an open cell e, it contains the whole closure e‾. A relative CW complex (X,A) is formed from the subcomplex A by attaching cells in stages; thus A↪X is a cellular inclusion. (Skeleta, CW subcomplexes, and relative CW complexes)

Proof

1.1F1F2F3

By the skeletal definition F3, collapsing Fr−1 leaves a wedge of one r-sphere per relative cell, using the disjoint-basepoint convention when Fr−1 is empty. Quotient identification and arbitrary wedge additivity in F2, followed by F1, show hk(Fr,Fr−1) is zero for k≠r and the stated direct sum for k=r. This includes no cells and zero-dimensional cells.

1.2F2

Write δr:hr(Fr,Fr−1)→hr−1(Fr−1,A) for the triple boundary and ρr:hr(Fr,A)→hr(Fr,Fr−1) for the quotient map. The differential is dr=ρr−1δr. Exactness of the triple (Fr−1,Fr−2,A) gives δr−1ρr−1=0.

2.1F2step 1.2algebra∎

Consequently dr−1dr=ρr−2(δr−1ρr−1)δr=0 for r≥2; for r=1 it holds because d0=0. A cellular map preserves each Fr and all natural triple maps, so it commutes with these differentials. No sphere-map incidence identification has been used.

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Sources