Signature of a knot

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The signature of a knot is a topological invariant in knot theory. It may be computed from the Seifert surface.

Given a knot K in the 3-sphere, it has a Seifert surface S whose boundary is K. The Seifert form of S is the pairing ϕ:H1(S)×H1(S) given by taking the linking number lk(a+,b) where a,bH1(S) and a+,b indicate the translates of a and b respectively in the positive and negative directions of the normal bundle to S.

Given a basis b1,...,b2g for H1(S) (where g is the genus of the surface) the Seifert form can be represented as a 2g-by-2g Seifert matrix V, Vij=ϕ(bi,bj). The signature of the matrix V+Vt, thought of as a symmetric bilinear form, is the signature of the knot K.

Slice knots are known to have zero signature.

The Alexander module formulation

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Knot signatures can also be defined in terms of the Alexander module of the knot complement. Let X be the universal abelian cover of the knot complement. Consider the Alexander module to be the first homology group of the universal abelian cover of the knot complement: H1(X;). Given a []-module V, let V denote the []-module whose underlying -module is V but where acts by the inverse covering transformation. Blanchfield's formulation of Poincaré duality for X gives a canonical isomorphism H1(X;)H2(X;) where H2(X;) denotes the 2nd cohomology group of X with compact supports and coefficients in . The universal coefficient theorem for H2(X;) gives a canonical isomorphism with Ext[](H1(X;),[]) (because the Alexander module is []-torsion). Moreover, just like in the quadratic form formulation of Poincaré duality, there is a canonical isomorphism of []-modules Ext[](H1(X;),[])Hom[](H1(X;),[[]]/[]), where [[]] denotes the field of fractions of []. This isomorphism can be thought of as a sesquilinear duality pairing H1(X;)×H1(X;)[[]]/[] where [[]] denotes the field of fractions of []. This form takes value in the rational polynomials whose denominators are the Alexander polynomial of the knot, which as a []-module is isomorphic to []/ΔK. Let tr:[]/ΔK be any linear function which is invariant under the involution tt1, then composing it with the sesquilinear duality pairing gives a symmetric bilinear form on H1(X;) whose signature is an invariant of the knot.

All such signatures are concordance invariants, so all signatures of slice knots are zero. The sesquilinear duality pairing respects the prime-power decomposition of H1(X;)—i.e.: the prime power decomposition gives an orthogonal decomposition of H1(X;). Cherry Kearton has shown how to compute the Milnor signature invariants from this pairing, which are equivalent to the Tristram-Levine invariant.

See also

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References

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  • C.Gordon, Some aspects of classical knot theory. Springer Lecture Notes in Mathematics 685. Proceedings Plans-sur-Bex Switzerland 1977.
  • J.Hillman, Algebraic invariants of links. Series on Knots and everything. Vol 32. World Scientific.
  • C.Kearton, Signatures of knots and the free differential calculus, Quart. J. Math. Oxford (2), 30 (1979).
  • J.Levine, Knot cobordism groups in codimension two, Comment. Math. Helv. 44, 229-244 (1969)
  • J.Milnor, Infinite cyclic coverings, J.G. Hocking, ed. Conf. on the Topology of Manifolds, Prindle, Weber and Schmidt, Boston, Mass, 1968 pp. 115–133.
  • K.Murasugi, On a certain numerical invariant of link types, Trans. Amer. Math. Soc. 117, 387-482 (1965)
  • A.Ranicki On signatures of knots Slides of lecture given in Durham on 20 June 2010.
  • H.Trotter, Homology of group systems with applications to knot theory, Ann. of Math. (2) 76, 464-498 (1962)

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