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LemmaStatement: Literature-sourcedProof: AI-generatedPipeline-generatedverified 2026-10-22 (gpt-6.1-sol)
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The positive-push Seifert pairing is well-defined for a link surface

Statement

Assume full AC. Let L be a nonempty smooth oriented link in the oriented 3-sphere, and let F be a connected compact smooth oriented embedded surface with oriented boundary L. For disjoint oriented embedded circles C,D⊂S3, define lk⁡(C,D) as the coefficient of the positive meridian of D in H1(S3∖D;Z), and extend it bilinearly to finite integral sums of oriented circles. This linking number is symmetric on disjoint circle cycles. Every class of H1(F;Z) has a representative that is a finite integral sum of pairwise disjoint smooth oriented embedded circles in F. The positive push-off x+ of such a representative is a sufficiently small copy in the positive normal direction determined by the ambient and surface orientations. For representatives x and y, the sum of the pairwise linking numbers between x+ and y depends only on [x] and [y], is independent of the sufficiently small positive push-off level, and is bilinear. Hence it defines the positive-push Seifert pairing on H1(F;Z).

Facts & Assumptions

Given: Full AC, a nonempty oriented link L, and a connected compact oriented spanning surface F with boundary L.

[A1]

Full AC is assumed; it implies dependent choice and countable choice, discharging the choice hypotheses of the compact-surface and Alexander-duality suppliers. The Axiom of Choice, AC implies DC implies countable choice, The Axiom of Countable Choice (ACω), The one-variable Alexander module of an oriented link

[F1]

The compact surface has a finite cellulation, and its first homology is finitely generated and represented by integral cellular cycles. Finite surface normal forms, Jordan disks, and torsion control

[F2]

Linking of disjoint oriented circles is the meridian coefficient; when a regular diagram and spanning surface are supplied it agrees with the signed intersection and mixed-crossing half-sum. The one-variable Alexander module of an oriented link, Linking number equals signed intersection with a spanning surface

[F3]

After moving a finite oriented link off infinity, it has a regular projection, a finite decorated immersion with finitely many mixed crossings. Oriented links in the three-sphere and ambient isotopy, Regular oriented link diagrams, Existence of regular projections

[F4]

Every smooth oriented circle has a supplied connected compact oriented spanning surface, so the link-intersection theorem applies to it. Every smooth oriented knot in S3 bounds a Seifert surface

[F5]

Here is the small-perturbation consequence needed below, derived from the construction in the proofs of The transversality homotopy theorem and Relative transversality preserves a map on a closed good region. If ∂Σ=D and C∩D=∅, work in N=S3∖D; then Z=Int⁡Σ is a closed embedded submanifold of N. Those proofs construct a smooth family G:S1×B→N with G0=C and transverse slices for parameters outside a null set. Such parameters occur arbitrarily near 0, and compactness of S1 gives Ga→C in C1. Sufficiently close maps remain embeddings: on finitely many small coordinate arcs a coordinate derivative stays bounded away from zero, while pairs outside a fixed diagonal neighbourhood retain a positive separation. Thus, for small good a, the whole path Gta consists of embeddings in N and its endpoint is transverse to Z. This proves the required perturbation through disjoint embedded circles without applying transversality to a surface with boundary.

Proof

Given: Full AC, L, and F as in the Statement.

1.1A1F1givenconstruct

Fix a finite cellulation of F from [F1]. An integral cellular 1-cycle represents each class of H1(F;Z). Replace each edge with coefficient n by ∣n∣ parallel oriented copies, reversing orientation when n<0. At each vertex the cycle condition says that incoming and outgoing copies occur in equal number. Around the boundary of a small vertex disk there is therefore an adjacent incoming/outgoing pair; join that pair by a small arc and delete its endpoints, repeating finitely until all endpoints are paired. The resulting arcs can be chosen disjoint in the disk and oriented consistently with the copies. Each smoothing changes the chain only by the boundary of a 2-chain in that disk. The result is a finite disjoint union of oriented embedded circles representing the original homology class.

1.2F2givenalgebra

For representatives X,X′ of the same class in H1(F;Z), there is an integral singular 2-chain A in F with ∂A=X−X′. Push the chain through a small positive normal level of F; its boundary is X+−X′+ and it is disjoint from any representative Y⊂F. Thus X+ and X′+ represent the same class in H1(S3∖Y;Z), so their meridian-coordinate linking sums with Y agree. Varying the small positive level traces an annulus in the positive bicollar, also disjoint from Y, and gives the same class.

1.3F2F3F4F5givenalgebra

If Y,Y′ represent the same class, choose an integral 2-chain B in F with ∂B=Y−Y′. For each circle component of X+ and each circle component of Y−Y′, [F4] supplies a spanning surface and [F5] permits a homotopy of the other circle in its complement to make it transverse to that surface while remaining an embedded circle. By [F3] choose a regular diagram of the pair. By [F2], linking is the half-sum of mixed crossing signs; exchanging the two components leaves the same mixed crossings with the same signs, so linking is symmetric. Bilinearity then gives lk⁡(X+,Y−Y′)=lk⁡(Y−Y′,X+). The cycle Y−Y′ bounds B in S3∖X+, so its total meridian coefficient there is zero. Hence the two linking sums agree in the second variable as well. Additivity of meridian coefficients gives bilinearity in both variables.

2.1step 1.1step 1.2step 1.3algebra∎

The value in the Statement is therefore independent of the chosen cycle representatives and push-off level and is bilinear on homology. In any ordered integral basis its matrix entries are Vij=lk⁡(ai+,aj), as required.

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