Vassiliev Invariant

Vassiliev invariants, discovered around 1989, provided a radically new way of looking at knots. The notion of finite type (a.k.a. Vassiliev) knot invariants was independently invented by V. Vassiliev and M. Goussarov around 1989. Vassiliev's approach is based on the study of discriminants in the (infinite-dimensional) spaces of smooth maps from one manifold into another. By definition, the discriminant consists of all maps with singularities.

For example, consider the space of all smooth maps from the circle into three-space . If is an embedding (i.e., has no singular points), then it represents a knot. The complement of the set of all knots is the discriminant . It consists of all smooth maps from into that have singularities, either local, where , or nonlocal, where is not injective. Two knots are equivalent iff they can be joined by a path in the space that does not intersect the discriminant. Therefore, knot types are in one-to-one correspondence with the connected components of the complement , and knot invariants with values in an Abelian group are nothing but cohomology classes from . The filtration of by subspaces corresponding to singular knots with a given number of ordinary double points gives rise to a spectral sequence, which contains, in particular, the spaces of finite type invariants.

Birman and Lin (1993) have contributed significantly to the simplification of the Vassiliev's original techniques. In particular, they explained the relation between Jones polynomials and finite type invariants (Peterson 1992, Birman and Lin 1993, Bar-Natan 1995) and emphasized the role of the algebra of chord diagrams. In fact, substituting the power series for as the variable in the Jones polynomial yields a power series whose coefficients are Vassiliev invariants (Birman and Lin 1993). Kontsevich (1993) proved the first difficult theorem about Vassiliev invariants with the help of the Kontsevich integral. Bar-Natan undertook a thorough study of Vassiliev invariants; in particular, he showed the importance of the algebra of Feynman diagrams and diagrams with uni- and tri-valent vertices (Bar-Natan 1995). Bar-Natan (1995) remains the most authoritative source on the subject.

Expressed in simple terms, Vassiliev's fundamental idea is to study the prolongation of knot invariants to singular knots--immersions having a finite number of ordinary double points. Let denote the set of equivalence classes of singular knots with double points and no other singularities. The following definition is based on a recursion which allows to extend a knot invariant from to , then to , etc., and thus finally to the whole of . Given a knot invariant , its Vassiliev prolongation is defined as by the rules

1. , and

2. Vassiliev's skein relation, illustrated below.

The right-hand side of Vassiliev's skein relation refers to the two resolutions of the double point--positive and negative. A crucial observation is that each of them is well-defined (does not depend on the plane projection used to express this relation). A knot invariant is called a Vassiliev invariant of order if its prolongation vanishes on all knots with more than double points. For example, the simplest nontrivial Vassiliev invariant has the following explicit description. Let be an arbitrary knot diagram of the given knot and an arbitrary distinguished point on , different from all crossings. Then

where the summation spreads over all pairs of crossing points such that (1) during one complete turn of the diagram in the positive direction starting from point the points and are encountered in the order , and (2) the four corresponding passages through these crossing points are underpass, overpass, overpass, and underpass, respectively. The numbers , stand for the local writhe at points and , defined according to the above illustration.

It turns out that the th coefficient of the Conway polynomial is a Vassiliev invariant of order and, in particular, the second coefficient coincides with .

Vassiliev invariants are at least as strong as all known polynomial knot invariants: Alexander, Jones, Kauffman, and HOMFLY polynomials. This means that if two knots and can be distinguished by such a polynomial, then there is a Vassiliev invariant that takes different values for and .

The set of all -valued Vassiliev invariants forms a vector space over the rationals, with the increasing filtration . The associated graded space has a structure of a Hopf algebra and can be interpreted as the algebra of chord diagrams.

The numbers of independent Vassiliev invariants of a given degree (i.e., the dimension of ) are known for to 12 (Kneissler 1997) and are summarized in following table (A007473).

	0	1	2	3	4	5	6	7	8	9	10	11	12
	1	1	2	3	6	10	19	33	60	104	184	316	548

The totality of all Vassiliev invariants is equivalent to one universal Vassiliev invariant defined through the Kontsevich integral.

Two of the most important problems about Vassiliev invariants were raised in 1990 and remain unanswered today.

1. Is it true that Vassiliev invariants distinguish knots? In other words, given two nonequivalent knots and , is it always possible to indicate a finite type invariant such that ?

2. Is it true that Vassiliev invariants can detect knot orientation? More specifically, is there a knot and a finite type invariant such that , where differs from by a change of parameterization that reverses the orientation?

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