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The torsion linking pairing of a rational homology sphere is nonsingular

Statement

Assume AC. If Y is a closed connected oriented 3-manifold with finite H1(Y;Z), then the bounding-chain torsion linking pairing λY is symmetric and nonsingular: its adjoint H1(Y;Z)→Hom⁡(H1(Y;Z),Q/Z) is an isomorphism.

Facts & Assumptions

Given: Full AC and a closed connected oriented 3-manifold Y with finite H1(Y;Z).

[A1]

Full AC is assumed wherever the cover and orientation conventions use the choice axiom. The Axiom of Choice

[F1]

Poincaré duality for closed oriented manifolds gives H2(Y;Z)≅H1(Y;Z) and H2(Y;Q)≅H1(Y;Q). Poincaré duality for oriented topological manifolds

[F2]

The cohomology universal coefficient sequence over Z identifies H1(Y;Q) with Hom⁡(H1(Y;Z),Q) and H1(Y;Q/Z) with Hom⁡(H1(Y;Z),Q/Z), since H0(Y;Z)=Z is free. The universal coefficient theorem for cohomology over a PID

[F3]

The coefficient sequence 0→Z→Q→Q/Z→0 gives the long exact cohomology sequence and its natural Bockstein map β:H1(Y;Q/Z)→H2(Y;Z). The long exact sequence in cohomology

[F4]

External triangulation input. A compact topological 3-manifold admits a finite manifold triangulation (Moise's theorem, as stated in Aschenbrenner–Friedl–Wilton, Theorem 3.1, p. 211, under their compact-manifold convention, p. 203). We use its barycentric dual cells as a chain model, not as an additional smoothness hypothesis on Y. Orient a dual cell so that its oriented transverse intersection with the corresponding primal cell is positive. The dual-cell description of Poincaré duality is recalled in Hatcher, §3.3, pp. 232–233; the specific bounding-chain/Bockstein identity is proved below, rather than assumed.

[F5]

Cellular homology computes singular homology for every CW complex and every abelian coefficient group. Under [A1], cellular cochains compute singular cohomology for CW pairs with local coefficients, naturally for coefficient morphisms. Apply these comparisons to the finite triangulation and its dual CW complex, the pair (Y,∅), and the trivial coefficient systems Z, Q and Q/Z. Thus cellular cycles and bounding chains represent precisely the singular homology classes, and the cellular coefficient-sequence Bockstein and evaluation agree with their singular counterparts. Cellular homology computes singular homology Cellular cochains compute cohomology with local coefficients

Proof

1.1F1F2F3givenalgebraA1

Since H1(Y;Z) is finite, H1(Y;Q)=0 by [F2], and H2(Y;Q)=0 by [F1]. Exactness of [F3] therefore makes β:H1(Y;Q/Z)→H2(Y;Z) an isomorphism. Write PD⁡:H1(Y;Z)→H2(Y;Z) for inverse cap duality.

1.2givenconstructalgebra

We first fix the intersection sign and verify independence directly. For transverse oriented 2-chains C,T in an oriented 3-manifold, orient their intersection so that ∂(C∩T)=(∂C)∩T−C∩(∂T). This sign follows by the outward-normal-first boundary convention in an oriented coordinate ball: taking a boundary in the second sheet passes its outward normal past the one normal direction of the first sheet. Consequently, the total signed endpoint count gives C⋅∂T=(∂C)⋅T. These identities extend linearly to chains; the terms on paired interior faces cancel. For a closed 2-chain E and torsion cycle y, choose m>0 and ∂T=my. Then m(E⋅y)=E⋅∂T=0, so E⋅y=0. Thus if ∂C=nx and ∂C′=n′x, the closed chain n′C−nC′ has zero intersection with y, giving (C⋅y)/n=(C′⋅y)/n′. Replacing x by x+∂S permits replacing C by C+nS and changes the quotient by the integer S⋅y. Replacing y by y+∂T changes it by (C⋅∂T)/n=x⋅T, also an integer. A change of transverse position is a chain homotopy: its prism has the moved-chain difference as boundary, so these same boundary identities apply. Hence the expression defines a pairing on the stated homology classes, independent of all these choices modulo Z.

2.1F1F4F5step 1.2construct

To identify that pairing with the Bockstein, use [F4] and [F5] and represent x by a primal cellular 1-cycle a, and y by a dual cellular 1-cycle b. Since n[a]=0, there is an integral primal cellular 2-chain C with ∂C=na. The dual-cell pairing gives the rational cellular 1-cochain u(e)=C⋅en on every oriented dual edge e. Let za be the integral cellular 2-cochain on the dual complex defined by za(σ)=a⋅σ. The sign convention in step 1.2 gives, for every dual 2-cell σ, (δu)(σ)=C⋅∂σn=(∂C)⋅σn=a⋅σ=za(σ). There is no extra minus sign: in an oriented chart with a tangent to the first coordinate and its dual 2-cell tangent to the second and third coordinates, a⋅σ=+1. A primal 2-cell followed by its positive transverse dual edge likewise has intersection +1. These are precisely the oriented dual-cell representatives of inverse cap duality, so [za]=PD⁡(x).

3.1F2F3F4F5step 1.1step 1.2step 2.1construct

Reducing u modulo Z gives a cocycle uˉ, because δu=za is integral. Under the natural comparison [F5], the connecting map in [F3] is constructed by lifting this cocycle to a rational cochain and taking its coboundary; therefore β[uˉ]=[δu]=PD⁡(x),⟨[uˉ],y⟩=u(b) mod Z=C⋅bn mod Z. By step 1.2 this is also the bounding-chain expression for any representatives and any bounding multiple in the definition. Cellular representatives cause no restriction by [F5]: cellular and singular chain models represent the same classes, and changes of representatives and transverse positions have already been accounted for. Thus the precise identity is λY(x,y)=⟨β−1PD⁡(x),y⟩. The evaluation is on the homology class y, not on a cohomology class called its Poincaré dual; equivalently it is the corresponding degree-3 cup-product evaluation on [Y].

4.1F1F2step 1.1step 3.1algebra

Under [F2], evaluation identifies H1(Y;Q/Z) with the entire character group Hom⁡(H1(Y;Z),Q/Z). The displayed identity in step 3.1 identifies the adjoint of the bounding-chain pairing with the composite of this isomorphism, β−1, and PD⁡. All three are isomorphisms, so the pairing is nonsingular. In particular its bilinearity also follows from these homomorphisms and evaluation.

5.1step 1.2step 3.1givenconstructalgebra∎

For torsion classes x,y, choose transverse representatives and chains C,D with ∂C=nx and ∂D=my. The boundary identity of step 1.2 applied to C∩D gives n(x⋅D)=m(C⋅y). Interchanging a 1-cycle and a 2-chain in an oriented 3-manifold changes the intersection sign by (−1)(3−1)(3−2)=+1, so x⋅D=D⋅x. Divide by nm and reduce modulo Z to obtain λY(x,y)=λY(y,x). This proves symmetry with the signed bounding-chain convention of the definition.

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