Alphabeta Math
LemmaStatement: Literature-sourcedProof: AI-generatedPipeline-generatedjudge pass (gpt-6-luna)verified 2026-10-22 (gpt-6.1-sol)
How statement and proof provenance work

The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.

  • Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
  • AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
  • AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.

These labels describe origin, not correctness: citations and verification chips remain separate evidence.

Seifert matrices of a knot are S-equivalent

Statement

Assume full AC. Let K be a smooth oriented knot in the oriented standard 3-sphere, and let F,F′ be any connected compact smooth oriented spanning surfaces for K. For any ordered integral bases of H1(F;Z) and H1(F′;Z), the matrices of the positive-push Seifert pairing are related by a finite sequence of integral unimodular congruences and the two rank-two elementary Seifert enlargements or their reverses.

Facts & Assumptions

Given: Full AC, a smooth oriented knot K, two connected smooth oriented spanning surfaces F,F′, and ordered integral bases for their first homology groups.

[A1]

Full AC is the choice-function axiom assumed by the knot Seifert-pairing interface. The Axiom of Choice

[F1]

The positive-push pairing is Vij=lk⁡(ai+,aj) and is bilinear on integral homology classes. Seifert pairing and matrix of an oriented knot, Well-definedness of the Seifert pairing

[F2]

If an ambient isotopy carries one oriented knot-surface pair to another, the transported basis has the same Seifert matrix; changing an integral basis gives a unimodular congruence. Seifert matrices of ambient-isotopic pairs are S-equivalent

[F3]

An arc surgery replaces two disks by the lateral annulus of a product cylinder while preserving the oriented boundary knot. Embedded arc surgery on a spanning surface

[F4]

The two elementary enlargement matrices are E0(V;x,y,z) and E1(V;x,y,z) as defined in S-equivalence. S-equivalence of integral Seifert matrices

[F6]

For disjoint oriented knots, linking is the signed intersection with a spanning surface and is symmetric in the two components; the mixed-crossing formula gives the same half-sum after the components are interchanged. Linking number equals signed intersection with a spanning surface

[F7]

The skew part of the positive-push Seifert matrix is the oriented intersection form on the surface. The skew part of a Seifert matrix is the surface intersection form

[L1]

Any two such surfaces are connected by finitely many ambient isotopies fixing the boundary and embedded arc surgeries or their reverses. Seifert surfaces of the same link are connected by arc surgeries

Proof

1.1A1F1F2F4givenalgebra

At an isotopy step in the finite surface sequence of [L1], [F2] gives equality of the matrices in the transported basis. If the target basis is changed by P∈GL2g(Z), bilinearity gives V′=PTVP, which is one of the defining S-equivalence moves by [F4].

1.2A1F1F3F4F6F7givenconstruct

Consider one arc surgery in that sequence. Choose the old basis curves away from the two surgery disks. The added product cylinder contributes a longitudinal class b and a meridian class c; together with the old basis these form an integral basis of the new surface because the surgery adds one orientable handle and hence two first-homology generators. In a cross-section {t0}×D2 of the cylinder, c={t0}×∂D2 bounds the disk D={t0}×D2 and the longitudinal class b meets D once. The disk and its parallel copies miss the old curves and their positive push-offs, so both pairings between c and every old basis curve vanish. If the positive normal of the lateral annulus points outward from the cylinder, b+ misses D and the slightly larger disk bounded by c+ meets b once; hence [F6] gives V(b,c)=0 and V(c,b)=±1. If that normal points inward, the smaller disk bounded by c+ misses b, while b+ crosses D once, giving V(c,b)=0 and V(b,c)=±1. Orient c so the single nonzero entry is +1. The same disks show V(c,c)=0. The tube core has integer self-linking z=V(b,b), and its pairings with the old curves give integer column and row vectors x and yT. By [F7], the difference between the two new cross entries equals the oriented intersection of the same ordered basis curves, so this is exactly one of E0(V;x,y,z) or E1(V;x,y,z), up to an integral basis change.

2.1F2F3F4L1step 1.1step 1.2construct∎

Apply [L1] to obtain a finite sequence of isotopies and arc surgeries or their reverses from F to F′. Steps 1.1 and 1.2 turn every isotopy or forward surgery into a defining S-equivalence move, and reverse surgery gives its inverse. Their finite composition, including initial and final basis changes, proves the statement.

Depends on

Used by

Dependency tree · two levels

50 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.

Sources