Linking form

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This page has not been refereed. The information given here might be incomplete or provisional.


1 Background: intersection forms

After Poincaré and Lefschetz, a closed oriented manifold N^{n} has a bilinear intersection form defined on its homology. Given a {k}--chain p \in C_{k}(N;\mathbb{Z}) and an (n-k)--chain q \in C_{n-k}(N;\mathbb{Z}) which is transverse to q, the signed count of the intersections between p and q gives an intersection number \langle\, p \, , \, q\, \rangle \in \mathbb{Z}.


The intersection form is defined by

\displaystyle I_N \colon H_k(N;\mathbb{Z}) \times H_{n-k}(N;\mathbb{Z}) \to  \mathbb{Z}; ([p],[q]) \mapsto  \langle p, q \rangle

and is such that

\displaystyle I_N(x,y) = (-)^{k(n-k)}I_N(y,x).

2 Definition of the linking form

By bilinearity, the intersection form vanishes on the torsion part of the homology. The analogue of the intersection pairing for the torsion part of the homology of a closed oriented manifold N^n is the bilinear \mathbb{Q}/\mathbb{Z}--valued linking form, which is due to Seifert:

\displaystyle L_N \colon TH_{\ell}(N;\mathbb{Z}) \times TH_{n-\ell-1}(N;\mathbb{Z}) \to \mathbb{Q}/\mathbb{Z}

such that

\displaystyle L_N(x,y) = (-)^{\ell(n-\ell-1)}L_N(y,x).


Given [x] \in TH_\ell(N;\mathbb{Z}) and [y] \in TH_{n-\ell-1}(N;\mathbb{Z}) represented by cycles x \in C_\ell(N;\mathbb{Z}) and y \in C_{n-\ell-1}(N,\mathbb{Z}), let w \in C_{\ell+1}(N;\mathbb{Z}) be such that \partial w = sy, for some s \in \mathbb{Z}. Then we define:

\displaystyle L_N([x],[y]) := \langle x, w \rangle/s \in \mathbb{Q}/\mathbb{Z}.

The resulting element is independent of the choices of x,y,w and s.

As an example, let N = \mathbb{RP}^3, so that \ell=1 and n=3. Now H_1(\mathbb{RP}^3;\mathbb{Z}) \cong \mathbb{Z}_2. Let \theta \in H_1(\mathbb{RP}^3;\mathbb{Z}) be the non--trivial element. To compute the linking L_{\mathbb{RP}^3}(\theta,\theta), consider \mathbb{RP}^3 modelled as D^3/\sim, with antipodal points on \partial D^2 identified, and choose two representative 1--chains x and y for \theta. Let x be the straight line between north and south poles and let y be half of the equator. Now 2y = \partial w, where w \in C_2(\mathbb{RP}^3;\mathbb{Z}) is the 2-disk whose boundary is the equator. We see that \langle x,w \rangle = 1, so that

\displaystyle L_{\mathbb{RP}^3}(\theta,\theta) = L_{\mathbb{RP}^3}([x],[y]) = \langle x,y \rangle/2 = 1/2.


3 References

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