TheoremComplete

Alexander Duality

Alexander duality relates the homology of a subspace of the sphere to the cohomology of its complement, providing a powerful tool for computing the topology of complements of embedded submanifolds.


The Theorem

Theorem8.9Alexander Duality

Let KK be a compact, locally contractible, nonempty, proper subspace of SnS^n. Then for all qq, there is an isomorphism H~q(K;Z)H~nq1(SnK;Z)\tilde{H}^q(K; \mathbb{Z}) \cong \tilde{H}_{n-q-1}(S^n \setminus K; \mathbb{Z}) where H~\tilde{H} denotes reduced (co)homology.

The proof combines Poincare-Lefschetz duality with excision. Consider the compact manifold with boundary obtained by removing a small open neighborhood of KK from SnS^n; Lefschetz duality for this manifold, combined with a limit argument, yields Alexander duality.


Classical Applications

ExampleJordan Curve Theorem

Let KS1K \cong S^1 be a simple closed curve in S2S^2. Alexander duality gives H~0(S2K)H~1(S1)Z\tilde{H}_0(S^2 \setminus K) \cong \tilde{H}^1(S^1) \cong \mathbb{Z} Since H~0\tilde{H}_0 measures one fewer than the number of path components, S2KS^2 \setminus K has exactly two path components. This is the Jordan Curve Theorem.

ExampleKnot complements

For a knot KS1K \cong S^1 embedded in S3S^3, Alexander duality gives:

  • H~0(S3K)H~2(S1)=0\tilde{H}_0(S^3 \setminus K) \cong \tilde{H}^2(S^1) = 0, so the complement is connected
  • H~1(S3K)H~1(S1)Z\tilde{H}_1(S^3 \setminus K) \cong \tilde{H}^1(S^1) \cong \mathbb{Z}
  • H~2(S3K)H~0(S1)Z\tilde{H}_2(S^3 \setminus K) \cong \tilde{H}^0(S^1) \cong \mathbb{Z}

All knot complements in S3S^3 have the same homology groups! The fundamental group π1(S3K)\pi_1(S^3 \setminus K), the knot group, provides the finer invariant needed to distinguish knots.


Generalization

Theorem8.10Alexander Duality for Manifolds

More generally, if MM is a closed oriented nn-manifold and KMK \subset M is a compact subspace, then Hq(K;Z)Hnq(M,MK;Z)H^q(K; \mathbb{Z}) \cong H_{n-q}(M, M \setminus K; \mathbb{Z}) When M=SnM = S^n and we use the long exact sequence of the pair (Sn,SnK)(S^n, S^n \setminus K) together with H~(Sn)=0\tilde{H}_*(S^n) = 0 for n* \neq n, this reduces to the classical form.

RemarkLinking numbers

Alexander duality provides the algebraic framework for defining linking numbers. If KK and LL are disjoint oriented closed curves in S3S^3, the linking number lk(K,L)\operatorname{lk}(K, L) is the image of [L][L] under the composition H1(S3K)H1(K)ZH_1(S^3 \setminus K) \cong H^1(K) \cong \mathbb{Z}. This integer measures how many times LL winds around KK and is a fundamental invariant in knot theory.

Alexander duality reveals a deep symmetry: the topology of a subspace and its complement in a sphere are intimately linked, with information about one completely determining the other at the level of homology.