What is a Singular Knot?

# What is a Singular Knot?

Zsuzsanna Dancso Zsuzsanna Dancso, School of Mathematics and Statistics
The Universit of Sydney
Sydney NSW 2006
Australia
###### Abstract.

A singular knot is an immersed circle in with finitely many transverse double points. The study of singular knots was initially motivated by the study of Vassiliev invariants. Namely, singular knots give rise to a decreasing filtration on the infinite dimensional vector space spanned by isotopy types of knots: this is called the Vassiliev filtration, and the study of the corresponding associated graded space has lead to many insights in knot theory. The Vassiliev filtration has an alternative, more algebraic definition for many flavours of knot theory, for example braids and tangles, but notably not for knots. This view gives rise to connections between knot theory and quantum algebra. Finally, we review results – many of them recent – on extensions of non-numerical knot invariants to singular knots.

## 1. Introduction

A singular knot is an immersed circle in , whose singularities are limited to finitely many transverse double points. We will restrict our attention to oriented singular knots, which are equipped with a direction: Figure 1 shows an example. Other knotted objects, such as braids, tangles, or knotted graphs have similar singular versions, see Figure 1 for an example of a singular braid. A singular knot diagram is a planar projection of a singular knot, which has two types of crossings: regular crossings with over/under strand information, and double points. Reidemeister moves can be formulated to describe singular knots modulo ambient isotopy, see Figure 2. For minimal sets of oriented Reidemeister moves see [BEHY]. Figure 1. An example of a 2-singular knot – that is, a knot with two double points; and a 3-singular braid on four strands. Figure 2. Reidemeister moves for singular knots, in addition to the usual Reidemeister 1, 2 and 3 moves.

## 2. The Vassiliev filtration

Singular knots give rise to a decreasing filtration, called the Vassiliev filtration on the infinite dimensional vector space generated by isotopy classes of knots. Knot invariants which vanish on some step of this filtration are called finite type or Vassiliev invariants. Examples include many famous knot invariants, for example the coefficients of any knot polynomial – after an appropriate variable substitution – are of finite type [BN1]. In this section we describe the Vassiliev filtration for knots and other knotted objects.

Let denote the set of (isotopy classes of) knots, and let be the -vector space111One may replace with one’s favourite field of characteristic zero, at no cost. spanned by elements of . In other words, elements of are formal linear combinations of knots.

Let denote the set of (isotopy classes of) -singular knots, and let . Each singularity of can be resolved two ways: by replacing the double point with an over-crossing, or with and under-crossing. Note that the notion of “over” and “under” crossings don’t depend on the choice of knot projection – this is true not only in but in any orientable manifold. We define a resolution map as follows: replace each singularity of by the difference of its two resolutions, as shown in Figure 3. This produces a linear combination of knots with coefficients, we call this the resolution of . By an abuse of notation, we denote also by the linear span of the image in .

The subspaces are a decreasing filtration on , called the Vassiliev filtration:

 (1) QK=K0⊃K1⊃K2⊃K3⊃...

It’s a worthwhile exercise to show that is the set of elements whose coefficients sum to zero:

 K1={∑iαiKi∈QK|∑iαi=0}.

When one encounters a filtered space, a natural idea is to study its associated graded space instead: this enables inductive arguments and degree-by-degree computations. The associated graded space of knots equipped with the Vassiliev filtration is, by definition, . The space has a useful combinatorial–diagrammatic description in terms of chord diagrams. The study of finite type invariants is closely tied to the study of the space .

We now examine the Vassiliev filtration from a more algebraic perspective through the example of braid groups. Recall that the braid group consists of braids on strands up to braid isotopy, and the group operation is given by vertical stacking. The Artin presentation is a finite presentation for the group in terms of generators and relations (see also Figure 4):

 Bn=⟨σ1,...,σn−1|σiσi+1σi=σi+1σiσi+1,andσiσj=σjσiwhen|i−j|≥2⟩.

Following the strands of a braid from bottom to top determines a permutation of points; this gives rise to a group homomorphism to the symmetric group. For example, (any resolution of) the braid of Figure 1 is mapped to the cycle . The image of a braid is called the skeleton of ; the kernel of this homomorphism is the pure braid group . The pure braid group also has a finite presentation due to Artin, in terms of the generators , shown in Figure 4, and somewhat more complicated relations. For more on pure braid presentations see [MM].

The Vassiliev filtration can be defined for braid groups the same way as it is defined for knots; we first discuss it for the pure braid group . In this case is the group algebra of the pure braid group over the field . Denote the linear subspace generated by the -image of -singular pure braids by . Just like in the case of knots, This is a two-sided ideal in , called the augmentation ideal.

However, in this case much more is true. Any -singular braid can be written as a product of -singular braids: one can “comb” the braid into horizontal levels so that each level has exactly one singularity. As a result, is simply the -th power of the ideal .

A similar statement holds for the braid group , with the difference that in the definition of linear combinations are only allowed within each coset of ; in other words, only braids of the same skeleton can be combined. Steps of the Vassiliev filtration once again correspond to powers of the augmentation ideal. In fact, this phenomenon is much more general. Many flavours of knotted objects can be finitely presented as an algebraic structure of some kind: tangles form a planar algebra; knotted trivalent graphs have their own special set of operations [Th]; virtual and welded tangles form circuit algebras [BD]. The Vassiliev filtration – or its appropriate generalizations – coincide with the powers of the augmentation ideal in all of these examples.

A notable exception is the case of knots. A “multiplication operation” does exist for knots: it is called connected sum and denoted ; see Figure 5 for a pictorial definition. It is not true, however, that any -singular knot is the connected sum of 1-singular knots. Knots which cannot be expressed as a non-trivial connected sum are called prime knots, and there exist prime knots of arbitrary crossing number, in particular all torus knots are prime. In other words, knots are not finitely generated as an “algebraic structure”.

The algebraic view outlined above gives rise to a deep connection between knot theory and quantum algebra. Let denote some class of knotted objects (such as knots, braids, tangles, etc). A central question in the study of finite type invariants is to find a universal finite type invariant, which contains all of the information that any finite type invariant can retain about . More precisely, a universal finite type invariant is a filtered map which takes values in the degree completed associated graded space, and which satisfies a certain universality property. Perhaps the most famous universal finite type invariant is the Kontsevich integral of knots [Ko]. It is still an open problem whether the Kontsevich integral separates knots.

Assume that some class of knotted objects forms a finitely presented algebraic structure with generators and relations (e. g.  may be the braid group). Assume one looks for a universal finite type invariant which respects operations in the appropriate sense (e. g.  may be an algebra homomorphism). Then it is enough to find the values of the generators , subject to equations arising from each . In other words, one needs to solve a set of equations in a graded space. This set of equations often turns out to be interesting in its own right: for knotted trivalent graphs or parenthesized tangles they are the equations which define Drinfeld associators in quantum algebra [MO, BN2, Da]; for welded foams they are the Kashiwara-Vergne equations of Lie theory [BD].

## 3. Invariants of singular knots

Vassiliev’s idea in the early ’90s was to extend number-valued knot invariants to singular knots using the resolution of singularities discussed above. This led to an explosion of activity in knot theory at the time. Since then singular knots have been studied in their own right by many researchers, and various non-numerical invariants have been extended to singular knots. Here we summarise some of these results.

In [MOY], Murakami, Ohtsuli and Yamada developed a skein theory for the HOMFLY polynomial using a generalisation of singular knots called abstract singular knots. We present a simplified version of their result, which is used in several applications. The HOMFLY polynomial is determined by the skein relation shown on the left of Figure 7, and its value on the unknot.

To define abstract singular knots, one replaces double points with an oriented thick edge from the incoming to the outgoing edges of the double point, creating an oriented trivalent graph embedded in , as in Figure 6. These trivalent graphs are called oriented abstract singular knots and they are characterised by two properties:

1. Each vertex is incident to one thick and two thin edges.

2. At each vertex the thin edges are oriented the same way, while the thick edge is oriented oppositely.

Embedded trivalent graphs which satisfy condition (1) are called abstract singular knots. Not every such abstract singular knot can be oriented to satisfy (2), and hence they don’t all arise from ordinary singular knots with double points: an example is shown in Figure 6. Figure 6. Creating an oriented abstract singular knot from a singular knot, and an abstract singular knot which cannot be oriented.

Let be the one-variable spacialization of the HOMFLY polynomial with the substitution , . In particular, is the Alexander polynomial, and is the Jones polynomial. Then satisfies the skein relations shown on the right of Figure 7, reducing to the case of planar trivalent graphs, that is, abstract singular knots with no crossings. For these graphs [MOY] provide a further set of skein relations which uniquely determine the value of . Figure 7. The original HOMFLY skein relation on the left; the HOMFLY skein relations for abstract singular knots [MOY] on the right.

Khovanov and Rozansky [KR] use the [MOY] calculus, and the homological algebra of matrix factorizations, in their categorification of the polynomials . In [OSS], Ozsvath, Stipsitz and Szabo generalize knot Floer homology to abstract singular knots.

In [KV] Kauffman and Vogel extend the Kauffman polynomial to singular knots – in fact to knotted four-valent graphs with rigid vertices. In [JL] Juyumaya and Lambropoulou introduced a Jones-type invariant for singular knots, using the theory of singular braids and a Markov trace on Yokonuma–Hecke algebras. In [Fi], Fiedler extended the Kauffman state models of the Jones and Alexander polynomials to the context of singular knots.

Quandle-type invariants have been generalised and studied for singular knots and other types of knot-like objects (virtual knots, flat knots, pseudoknots). Authors who have contributed to this research include Churchill, Elhamdadi, Hajij, Henrich, Nelson, Oyamaguchi, and Sazdanovich [HN, NOS, CEHN].

This short summary can not aim to be a comprehensive treatment of the rich body of research, spanning nearly three decades, on singular knots and related knotted objects. We hope that the reader will be inspired to explore some of the many pointers and references, and contribute to the future of the subject.

## References

• [BN1] D. Bar-Natan: On the Vassiliev knot invariants, Topology 34 (1995) 423–472.
• [BN2] D. Bar-Natan: Non-associative tangles, Geometric Topology, proceedings of the Georgia international topology conference, W. H. Kazez, ed., 139–183, Amer. Math. Soc. and International Press, Providence, 1997.
• [BD] D. Bar-Natan, Z. Dancso: Finite type invariants of w-knotted objects II: tangles, foams and the Kashiwara–Vergne problem, Math. Annalen 367(3-4) 1517–1586.
• [BEHY] K. Bataineh, M. Elhamdadi, M. Hajij, and W. Youmans: Generating sets of Reidemeister moves of oriented singular links and quandles, arXiv:1702.01150.
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• [HN] A. Henrich and S. Nelson: Semiquandles and flat virtual knots, Pacific J. Math.  248 (2010), no. 1, 155–170.
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• [KR] M. Khovanov and L. Rozansky: Matrix factorizations and link homology, Fund. Math.  199-1 (2008), 1–91.
• [KV] L. H. Kauffman and P. Vogel: Link polynomials and a graphical calculus, J. Knot Theory Ramifications 1 (1992), no. 1, 59–104.
• [Ko] M. Kontsevich: Vassiliev’s knot invariants, Adv. Sov. Math.  16(2) (1993) 137–150.
• [MM] D. Margalit, J. McCammond: Geometric presentations of the pure braid group, J. Knot Theory Ramifications 18-1 (2009), 1–20.
• [MO] J. Murakami, T. Ohtsuki: Topological quantum field theory for the universal quantum invariant, Commun. Math. Phys.  188 (1997), 501–520.
• [MOY] H. Murakami, T. Ohtsuki and S. Yamada: HOMFLY polynomial via an invariant of coloured plane graphs, Enseign. Math.  2 44 (1998), no. 3-4, 325–360.
• [NOS] S. Nelson, N. Oyamaguchi, R. Sazdanovic: Psyquandles, singular knots and pseudoknots, arXiv:1710.08481.
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• [Th] D. P. Thurston: The algebra of knotted trivalent graphs and Turaev’s shadow world, Geom. Toplol. Monographs 4 (2002), 337–362.
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