A Seifert surface for an oriented knot is a compact connected oriented surface whose oriented boundary is . For homology classes represented by oriented curves , the Seifert form is
where is the positive normal push-off. Choosing a basis of gives a Seifert matrix .
For , the Levine-Tristram signature is
The determinant of this Hermitian matrix vanishes away from exactly at the unit roots of the Alexander polynomial of a knot . Consequently the signature is locally constant on their complement.
For near ,
The real skew-symmetric unimodular matrix has standard symplectic blocks, so the Hermitian matrix has its positive and negative eigenvalues in opposite pairs and has signature zero. Thus near . If has no unit roots, then contains no singular point of the signature form and is connected, so local constancy gives everywhere. With the usual convention , the signature vanishes identically.
Solved by gpt-5.6-sol high.
After replacing a class by a nonsingular representative, let represent a Seifert form over a field of characteristic different from two. Set
A direct calculation gives , so is an isometric structure. A metabolizer for corresponds to a -invariant metabolizer for , and stabilization gives the canonical homomorphism
Conversely, for an isometric structure with invertible, define
Then and . These constructions respect orthogonal sums and metabolic structures and are inverse on Witt classes, proving .
For an irreducible symmetric Laurent polynomial , the primary component of an isometric structure is
for large . The primary decomposition is orthogonal, so restriction of and to defines the projection
Now take and let have roots on the unit circle, with in the upper half-plane. The isomorphism sends a class to the even signature jump
For the class of a knot, this is precisely the jump of its Levine-Tristram signature at the root ; reversing the choice of side changes the overall sign convention.
Solved by gpt-5.6-sol high.
Seifert matrix Created 2026-09-24 Updated 2026-09-24
A Seifert matrix represents the Seifert form in an integral basis of . Its skew-symmetrization represents the intersection form of the surface and is unimodular.