ConceptComplete

Poincare Duality and Compactly Supported Cohomology

Poincare duality is one of the most profound results in topology, establishing a symmetry in the cohomology of oriented closed manifolds. Its proof in the de Rham setting uses integration to construct a non-degenerate pairing.


Compactly Supported Cohomology

Definition5.5Compactly supported de Rham cohomology

Let Ωck(M)\Omega^k_c(M) denote the space of compactly supported smooth kk-forms on MM. The compactly supported de Rham cohomology is

Hck(M)=ker(d:ΩckΩck+1)im(d:Ωck1Ωck).H^k_c(M) = \frac{\ker(d: \Omega^k_c \to \Omega^{k+1}_c)}{\operatorname{im}(d: \Omega^{k-1}_c \to \Omega^k_c)}.

For compact manifolds, Hck(M)=HdRk(M)H^k_c(M) = H^k_{\mathrm{dR}}(M). For non-compact manifolds, they differ.

ExampleCompactly supported cohomology of $\mathbb{R}^n$

Hck(Rn)RH^k_c(\mathbb{R}^n) \cong \mathbb{R} if k=nk = n and 00 otherwise. The generator of Hcn(Rn)H^n_c(\mathbb{R}^n) is any bump nn-form with total integral 1. This contrasts with HdRk(Rn)=0H^k_{\mathrm{dR}}(\mathbb{R}^n) = 0 for k1k \geq 1.


The Poincare Duality Pairing

Definition5.6Integration pairing

For a closed oriented nn-manifold MM, the integration pairing is the bilinear map

,:Hk(M)×Hnk(M)R,[α],[β]=Mαβ.\langle \cdot, \cdot \rangle: H^k(M) \times H^{n-k}(M) \to \mathbb{R}, \quad \langle [\alpha], [\beta] \rangle = \int_M \alpha \wedge \beta.

This is well-defined: if α=α+dη\alpha' = \alpha + d\eta, then Mαβ=Mαβ+Md(ηβ)=Mαβ\int_M \alpha' \wedge \beta = \int_M \alpha \wedge \beta + \int_M d(\eta \wedge \beta) = \int_M \alpha \wedge \beta by Stokes' theorem (since MM is closed).

Theorem5.4Poincare duality

If MM is a closed oriented nn-manifold, the integration pairing

HdRk(M)×HdRnk(M)RH^k_{\mathrm{dR}}(M) \times H^{n-k}_{\mathrm{dR}}(M) \to \mathbb{R}

is non-degenerate. In particular, Hk(M)(Hnk(M))H^k(M) \cong (H^{n-k}(M))^*, and if the cohomology is finite-dimensional, dimHk(M)=dimHnk(M)\dim H^k(M) = \dim H^{n-k}(M).


Consequences

ExampleSymmetry of Betti numbers

For a closed oriented nn-manifold, the Betti numbers satisfy bk=bnkb_k = b_{n-k}. For example:

  • S2S^2: b0=b2=1b_0 = b_2 = 1, b1=0b_1 = 0.
  • T2T^2: b0=b2=1b_0 = b_2 = 1, b1=2b_1 = 2.
  • CP2\mathbb{C}P^2: b0=b4=1b_0 = b_4 = 1, b2=1b_2 = 1, b1=b3=0b_1 = b_3 = 0.
RemarkPoincare duality for manifolds with boundary

For compact oriented manifolds with boundary, Poincare duality takes the form Hk(M)(Hnk(M,M))H^k(M) \cong (H^{n-k}(M, \partial M))^*, where H(M,M)H^*(M, \partial M) denotes relative cohomology (forms vanishing on M\partial M). This is the Lefschetz duality theorem.

Definition5.7Euler characteristic via Poincare duality

The Euler characteristic χ(M)=k=0n(1)kbk\chi(M) = \sum_{k=0}^n (-1)^k b_k satisfies χ(M)=0\chi(M) = 0 for odd-dimensional closed oriented manifolds (since bk=bnkb_k = b_{n-k} and the terms cancel in pairs). For even-dimensional manifolds, χ\chi is a fundamental topological invariant.

RemarkIntersection form

On a closed oriented 44-manifold M4M^4, Poincare duality restricts to a non-degenerate symmetric bilinear form on H2(M;Z)H^2(M; \mathbb{Z}), the intersection form. Freedman and Donaldson showed that this form determines the homeomorphism type (simply connected case) but not the diffeomorphism type, leading to the discovery of exotic smooth structures on R4\mathbb{R}^4.