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A table of nn-component handlebody links of genus n+1n+1 up to six crossings

Giovanni Bellettini Dipartimento di Ingegneria dell’Informazione e Scienze Matematiche, Università di Siena, 53100 Siena, Italy, and International Centre for Theoretical Physics ICTP, Mathematics Section, 34151 Trieste, Italy bellettini@diism.unisi.it Giovanni Paolini California Institute of Technology and Amazon Web Services, Pasadena CA, United States (work done while at University of Fribourg, Department of Mathematics, 1700 Fribourg, Switzerland) paolini@caltech.edu Maurizio Paolini Dipartimento di Matematica e Fisica, Università Cattolica del Sacro Cuore, 25121 Brescia, Italy maurizio.paolini@unicatt.it  and  Yi-Sheng Wang National Center for Theoretical Sciences, Mathematics Division, Taipei 106, Taiwan yisheng@ncts.ntu.edu.tw
Abstract.

A handlebody link is a union of handlebodies of positive genus embedded in 33-space, which generalizes the notion of links in classical knot theory. In this paper, we consider handlebody links with one genus 22 handlebody and n1n-1 solid tori, n>1n>1. Our main result is the complete classification of such handlebody links with six crossings or less, up to ambient isotopy.

1. Introduction

Knot tabulation has a long and rich history. Some early work, motivated by Kelvin’s vortex theory, dates back to as early as the late 19th. Over the past decades, more effort has been put into it by many physicists and mathematicians; all prime knots up to 1616 crossings are now classified [8]. In recent years knot tabulation has been further generalized to other contexts. [17] and [19] tabulate all prime theta curves and handcuff graphs up to seven crossings, [10] enumerates all irreducible handlebody knots of genus 22 up to six crossings, and [5] classifies all alternating Lengendrian knots up to seven crossings.

The aim of this paper is to extend the Ishii-Kishimoto-Moriuchi-Suzuki handlebody knot table [10] to handlebody links with n>1n>1 components having total genus n+1n+1. We call such a handlebody link an (n,1)(n,1)-handlebody link; it consists of exactly one genus 22 handlebody and n1n-1 solid tori. The following theorems summarize the main results of the paper.

Theorem 1.1.

Table 1 enumerates all non-split111A handlebody link HL{\rm HL} is split if there is a 22-sphere 𝔖𝕊3\mathfrak{S}\subset\mathbb{S}^{3} with 𝔖HL=\mathfrak{S}\cap{\rm HL}=\emptyset separating HL{\rm HL} into two parts., irreducible222A handlebody link HL{\rm HL} is reducible if there is a 22-sphere 𝔖\mathfrak{S} in 𝕊3\mathbb{S}^{3} with 𝔖HL\mathfrak{S}\cap{\rm HL} an incompressible disk in HL{\rm HL}. (n,1)(n,1)-handlebody links, up to ambient isotopy and mirror image, by their minimal diagrams, up to six crossings.

414_{1} and 515_{1} in Table 1 are the only non-split, irreducible (n,1)(n,1)-handlebody links with four and five crossings, respectively. There are 1515 handlebody links with six crossings, among which 88 have two components (n=2n=2), 66 have three components (n=3n=3), and 11 has four components (n=4n=4). As a side note, 656_{5} in Table 1 also represents the famous figure eight puzzle devised by Stewart Coffin [3]. Thus, its unsplittability implies the impossibility of solving the puzzle (Remark 3.2). Also, 696_{9} in Table 1 is an irreducible handlebody link with a \partial-irreducible complement; such phenomenon cannot happen when n=1n=1 (Remark 3.3).

Our task with respect to Table 1 is two-fold. Firstly we need to show that there is no extraneous entry, i.e. that all entries in the table

  • U.1

    represent non-split handlebody links,

  • U.2

    represent irreducible handlebody links,

  • U.3

    are mutually inequivalent, up to mirror image,

  • U.4

    attain minimal crossing numbers.

Secondly we have to prove that the table is complete; namely, there is no missing handlebody link with 66 crossings or less.

In Section 3 we prove U.1-U.3, making use of invariants such as the linking number [16], irreducibility criteria [2], and the Kitano-Suzuki invariant [13] (Theorems 3.2, 3.7, and 3.1, respectively). We prove the completeness of Table 1 by exhausting all—except for those obviously non-minimal—diagrams of non-split, irreducible (n,1)(n,1)-handlebody links up to six crossings (Section 4).

We first observe that the underlying plane graph of a diagram of a non-split, irreducible (n,1)(n,1)-handlebody link necessarily has edge connectivity equal to 22 or 33; for the sake of simplicity, such a diagram is said to have 22- or 33-connectivity, respectively. Diagrams with 33-connectivity up to six crossings are generated by a computer code, whereas to recover handlebody links represented by diagrams with 22-connectivity, we employ the knot sum—the order-22 vertex connected sum—of spatial graphs [17]. In more detail, a minimal diagram DD with 22-connectivity can be decomposed by decomposing circles333a circle that intersects DD at two different arcs. into simpler tangle diagrams, each of which induces a spatial graph that admits a minimal diagram with 33- or 44-connectivity, as illustrated in Fig. 1.1. This decomposition allows us to recover the handlebody link represented by DD by performing the knot sum between prime links and a spatial graph that admits a minimal diagram with 33-connectivity.

Refer to caption
decomposing circle
Refer to caption
knot sum of spatial graphs
Refer to caption
induced spatial graphs
Refer to caption
Figure 1.1. Decomposing a minimal diagram with 22-connectivity.

Once a list containing all possible minimal diagrams of non-split, irreducible handlebody links is produced, we examine each entry on the list manually (Appendix A), and show that either it is non-minimal or it represents a handlebody link ambient isotopic to one in Table 1, up to mirror image. This proves the completeness, and also implies U.4, given U.1-U.3.

Theorem 1.2.

All but 515_{1}, 636_{3}, 666_{6}, 676_{7}, 686_{8}, 6106_{10} in Table 1 are achiral.

The main tool used to inspect chirality is Theorem 5.3, where we prove a uniqueness result for the decomposition of non-split, irreducible handlebody links in terms of order-22 connected sum of handlebody-link-disk pairs (Definition 5.1).

Theorem 1.3.

Table 5 enumerates all non-split, reducible (n,1)(n,1)-handlebody links up to 66 crossings, up to mirror image.

Theorem 1.3 follows from the irreducibility of handlebody links in Table 1 and a uniqueness factorization theorem (Theorem 6.1) for non-split, reducible (n,1)(n,1)-handlebody links in terms of order-11 connected sum (Definition 6.1).

The structure of the paper is the following. Basic properties of handlebody links are reviewed in Section 2; uniqueness, unsplittability, and irreducibility of handlebody links in Table 1 are examined in Section 3. The completeness of the table is discussed in Section 4. Section 5 introduces the notion of decomposable handlebody links, which is used for examining the chirality of handlebody links in Table 1. Lastly, a complete classification of non-split, reducible handlebody links, up to 66 crossings, is given in Section 6. In the appendix we include an analysis on the output of the code, available at http://dmf.unicatt.it/paolini/handlebodylinks/.

Throughout the paper we work in the PL\operatorname{PL} category; for the illustrative purposes, the drawings often appear smooth. In the case of 33-dimensional submanifolds in 𝕊3\mathbb{S}^{3}, the PL\operatorname{PL} category is equivalent to the smooth category due to [4, Theorem 55], [7, Theorems 7.17.1, 7.47.4], [20, Theorem 8.88.8, 9.69.6, 10.910.9].

Table 1. Non-split, irreducible handlebody links up to six crossings.
[Uncaptioned image]

414_{1}     [Uncaptioned image]515_{1}
[Uncaptioned image]616_{1} [Uncaptioned image]626_{2} [Uncaptioned image]636_{3} [Uncaptioned image]646_{4}
[Uncaptioned image]656_{5} [Uncaptioned image]666_{6} [Uncaptioned image]676_{7} [Uncaptioned image]686_{8}
[Uncaptioned image]696_{9} [Uncaptioned image]6106_{10} [Uncaptioned image]6116_{11} [Uncaptioned image]6126_{12}
[Uncaptioned image]6136_{13} [Uncaptioned image]6146_{14} [Uncaptioned image]6156_{15}

2. Preliminaries

2.1. Handlebody links and spatial graphs

Definition 2.1 (Embeddings in 𝕊3\mathbb{S}^{3}).

A handlebody link HL{\rm HL} (resp. a spatial graph GG) is an embedding of finitely many handlebodies of positive genus (resp. a finite graph444A finite graph is a graph with finitely many vertices and edges; in addition, we require that no component has a positive Euler characteristic, to avoid trivial objects. A circle is regarded as a graph without vertices as in [9].) in the oriented 33-sphere 𝕊3\mathbb{S}^{3}.

The genus of a handlebody link is the sum of the genera of its components; a spatial graph is trivalent if the underlying graph is trivalent (each node has degree 3). By a slight abuse of notation, we also use HL{\rm HL} (resp. GG) to denote the image of the embedding in 𝕊3\mathbb{S}^{3}. Let rHLr{\rm HL} (resp. rGrG) be the mirror image of HL{\rm HL} (resp. GG).

Definition 2.2 (Equivalence).

Two handlebody links HL{\rm HL}, HL{\rm HL}^{\prime} (resp. spatial graphs G,GG,G^{\prime}) are equivalent if they are ambient isotopic; they are equivalent up to mirror image if HL{\rm HL} (resp. GG) is equivalent to HL{\rm HL}^{\prime} or rHLr{\rm HL}^{\prime} (resp. GG^{\prime} or rGrG^{\prime}).

A regular neighborhood of a spatial graph defines a handlebody link, up to equivalence [22, 3.243.24], and a spine of a handlebody link HL{\rm HL} is a spatial graph GG with HL{\rm HL} a regular neighborhood of GG [9]. In practice, it is more convenient to consider spines that are trivalent.

Lemma 2.1.

Every handlebody link admits a (trivalent) spine.

Proof.

It suffices to prove the connected case. We suppose HK\operatorname{HK} is a handlebody knot of genus gg, and 𝐃={D1,,D3g3}\mathbf{D}=\{D_{1},\cdots,D_{3g-3}\} is a set of disjoint incompressible disks in HK\operatorname{HK} such that the complement HKiN(Di)\operatorname{HK}\setminus\bigcup_{i}N(D_{i}) of their tubular neighborhoods N(Di)N(D_{i}) in HK\operatorname{HK} consists of 2(g1)2(g-1) 33-balls, each of which has non-trivial intersection with exactly three components of i=13g3N(Di)¯\coprod_{i=1}^{3g-3}\partial\overline{N(D_{i})}. Such a disk system always exists.

Let disks Di1,Di2,Di3D_{i1},D_{i2},D_{i3} be components of Bi(k=13g3N(Dk)¯)B_{i}\cap\big{(}\bigcup_{k=1}^{3g-3}\overline{N(D_{k})}\big{)}, and choose points vi1,vi2,vi3v_{i1},v_{i2},v_{i3} in the interior of Di1,Di2,Di3D_{i1},D_{i2},D_{i3} and a point viv_{i} in the interior of BiB_{i}. Then, join viv_{i} to vijv_{ij} by a path for each jj; this gives us a trivalent vertex. Repeat the construction for every ii, and then glue the vijv_{ij} together so that the vertices vijv_{ij} and vijv_{i^{\prime}j^{\prime}} are identified if they are in the same N(Dk)¯\overline{N(D_{k})}, for some kk. This way, we obtain a connected trivalent spine of HK\operatorname{HK} with 2(g1)2(g-1) trivalent vertices. ∎

In general, a trivalent spine of a nn-component handlebody link of genus gg has 2(gn)=2t2(g-n)=2t trivalent vertices, and we call such a handlebody link a (n,t)(n,t)-handlebody link. This paper is primarily concerned with the case t=1t=1.

2.2. Diagrams

Let 𝕊k=k\mathbb{S}^{k}=\mathbb{R}^{k}\cup\infty, and without loss of generality, it may be assumed handlebody links or spatial graphs are away from \infty.

Definition 2.3 (Regular projection).

A regular projection of a spatial graph GG is a projection π:𝕊3𝕊2\pi:\mathbb{S}^{3}\setminus\infty\rightarrow\mathbb{S}^{2}\setminus\infty such that the set π1(x)G\pi^{-1}(x)\cap G is finite with its cardinality #(π1(x)G)2\#(\pi^{-1}(x)\cap G)\leq 2 for any x𝕊2x\in\mathbb{S}^{2}\setminus\infty, and no 0-simplex of the polygonal subset GG of 𝕊3\mathbb{S}^{3} is in the preimage of a double point, a double point being a point x𝕊2x\in\mathbb{S}^{2}\setminus\infty with #(π1(x)G)=2\#(\pi^{-1}(x)\cap G)=2.

As with the case of knots, up to ambient isotopy, every spatial graph admits a regular projection: the idea is to choose a vector vv neither parallel to a 11-simplex in the polygonal subset G𝕊3=3G\subset\mathbb{S}^{3}\setminus\infty=\mathbb{R}^{3} nor in a plane containing a 0-simplex and a 11-simplex or two 11-simplices; then isotopy GG slightly to remove those points xx with #πv1(x)G>2\#\pi_{v}^{-1}(x)\cap G>2, where πv\pi_{v} is the projection onto the plane normal to vv.

Definition 2.4 (Diagram of a spatial graph).

A diagram of a spatial graph GG is the image of a regular projection of GG with relative height information added to each double point.

The convention is to make breaks in the line corresponding to the strand passing underneath; thus each double point becomes a crossing of the diagram.

Definition 2.5 (Diagram of a handlebody link).

A diagram of a handlebody link HL{\rm HL} is a diagram of a spine of HL{\rm HL}.

A diagram of GG (resp. HL{\rm HL}) is trivalent if it is obtained from a regular projection of a trivalent spatial graph (resp. spine).

Definition 2.6 (Crossing numbers).

The crossing number c(D)c(D) of a diagram DD of a handlebody link HL{\rm HL} (resp. of a spatial graph GG) is the number of crossings in DD. The crossing number c(HL)c({\rm HL}) of HL{\rm HL} (resp. c(G)c(G) of GG) is the minimum of the set

{c(D)D a diagram of HL (resp. G)}.\{c(D)\mid\text{$D$ a diagram of ${\rm HL}$ $($resp. $G)$}\}.
Definition 2.7 (Minimal diagram).

A minimal diagram DD of a handlebody link HL{\rm HL} (resp. of a spatial graph GG) is a diagram of HL{\rm HL} (resp. GG) with c(D)=c(HL)c(D)=c({\rm HL}) (resp. c(D)=c(G)c(D)=c(G)).

Every multi-valent vertex in a minimal diagram DD can be replaced with some trivalent vertices by the inverse of the contraction move [9, Fig. 11] without changing the crossing number, so for a handlebody link (resp. a spatial graph) there always exists a trivalent minimal diagram DD. From now on, we shall use the term “a diagram” to refer to a trivalent diagram of either a spatial graph or a handlebody link.

Observe that, regarding each crossing as a quadrivalent vertex, we obtain a plane graph, a finite graph embedded in the 22-sphere. In practice, we work backward and start with a plane graph having only trivalent and quadrivalent vertices, and produce diagrams by replacing quadrivalent vertices with under- or over-crossings. If the plane graph has 2t2t trivalent vertices and cc quadrivalent vertices, then we can recover 2c12^{c-1} diagrams from it, up to mirror image. In particular, a cc-crossing (n,t)(n,t)-handlebody link can be recovered from one of these plane graphs. Therefore if one can enumerate all plane graphs with 2t2t trivalent vertices and up to cc quadrivalent vertices, then one can find all (n,t)(n,t)-handlebody links up to cc crossings.

2.3. Moves

Definition 2.8 (Moves).

Local changes in a diagram depicted in Fig. 2.1 and Fig. 2.2 are called generalized Reidemeister moves, and the local change in Fig. 2.3 is called an IH-move.

Note that spines of equivalent handlebody links might be inequivalent as spatial graphs; indeed, the following holds.

Theorem 2.2 ([12, Theorem 2.12.1], [26]).

Two trivalent spatial graphs are equivalent if and only if their diagrams are related by a finite sequence of generalized Reidemeister moves.

Theorem 2.3 ([9, Corollary 22]).

Two handlebody links are equivalent if and only if their trivalent diagrams are related by a finite sequence of generalized Reidemeister moves and IH-moves.

Refer to caption
Refer to caption
Refer to caption
Figure 2.1. Classical Reidemeister moves of type I, II, III.
Refer to caption
Refer to caption
Figure 2.2. Reidemeister moves IV and V involve a triple point.
Refer to caption
Figure 2.3. The IH-move.

When analyzing the data from the code (Appendix A), it is more convenient to call a diagram IH-minimal if the number of crossings cannot be reduced by generalized Reidemeister moves and IH moves, that is, “minimal” as a diagram of a handlebody link, and to call a diagram R-minimal if the number of crossings cannot be reduced by generalized Reidemeister moves, that is, “minimal” as a diagram of a spatial graph.

2.4. Non-split, irreducible handlebody links

Definition 2.9 (Edge connectivity of a graph).

The edge-connectivity of a graph is the minimum number of edges whose deletion disconnects the graph.

Definition 2.10 (Connectivity of a diagram).

A diagram has ee-connectivity if its underlying plane graph has edge-connectivity ee.

Definition 2.11 (Split handlebody link).

A handlebody link HL{\rm HL} is split if there exists a 22-sphere 𝔖𝕊3\mathfrak{S}\subset\mathbb{S}^{3} such that 𝔖HL=\mathfrak{S}\cap{\rm HL}=\emptyset and both components of the complement 𝕊3𝔖¯\overline{\mathbb{S}^{3}\setminus\mathfrak{S}} have non-trivial intersection with HL{\rm HL}.

Definition 2.12 (Reducible handlebody link).

A handlebody link HL{\rm HL} is reducible if its complement admits a 22-sphere 𝔖\mathfrak{S} such that 𝔖HL\mathfrak{S}\cap{\rm HL} is an incompressible disk in HL{\rm HL}; otherwise it is irreducible.

Note that 𝔖\mathfrak{S} in Definition 2.12 factorizes HL{\rm HL} into two handlebody links, each called a factor of the factorization of HL{\rm HL}.

A diagram with 0-connectivity (resp. 11-connectivity) represents a split (resp. reducible) handlebody link, so only diagrams with connectivity greater than 11 are of interest to us; on the other hand, the connectivity of a diagram of a (n,t)(n,t)-handlebody link with t>0t>0 cannot exceed 33.

Now, we recall the order-22 vertex connected sum between spatial graphs [17], which is used to produce handlebody links represented by minimal diagrams with 22-connectivity. A trivial ball-arc pair of a spatial graph GG is a 33-ball BB with GBG\cap B a trivial tangle in BB; it is oriented if an orientation of GBG\cap B is given.

Definition 2.13 (Knot sum).

Given two spatial graphs G1,G2G_{1},G_{2} with oriented trivial ball-arc pairs B1,B2B_{1},B_{2} of G1,G2G_{1},G_{2}, respectively, their order-22 vertex connected sum (G1,B1)#(G2,B2)(G_{1},B_{1})\#(G_{2},B_{2}) is a spatial graph obtained by removing the interiors of B1,B2B_{1},B_{2} and gluing the resulting manifolds 𝕊3B1¯\overline{\mathbb{S}^{3}\setminus B_{1}} and 𝕊3B2¯\overline{\mathbb{S}^{3}\setminus B_{2}} by an orientation-reserving homoemorphism

h:((𝕊3B1¯),(G1B1))((𝕊3B2¯),(G2B2)).h:\big{(}\partial(\overline{\mathbb{S}^{3}\setminus B_{1}}\big{)},\partial(G_{1}\cap B_{1}))\rightarrow(\partial\big{(}\overline{\mathbb{S}^{3}\setminus B_{2}}\big{)},\partial(G_{2}\cap B_{2})).

The notation G1#G2G_{1}\#G_{2} denotes the set of order-22 vertex connected sums of G1,G2G_{1},G_{2} given by all possible trivial ball-arc pairs.

Since an order-22 vertex connected sum depends only on the edges of G1,G2G_{1},G_{2} intersecting with B1,B2B_{1},B_{2} and their orientations, G1#G2G_{1}\#G_{2} is a finite set.

3. Uniqueness, non-splittability, and irreducibility

Recall that, given a finite group 𝖦\mathsf{G}, the Kitano-Suzuki invariant ks𝖦(HL)ks_{\mathsf{G}}({\rm HL}) of a handlebody link HL{\rm HL} is the number of conjugate classes of homomorphisms from π1(𝕊3HL¯)\pi_{1}(\overline{\mathbb{S}^{3}\setminus{\rm HL}}) to 𝖦\mathsf{G} [13]. Table 2 lists the invariants ks𝖠4(HL)ks_{\mathsf{A}_{4}}({\rm HL}) and ks𝖠5(HL)ks_{\mathsf{A}_{5}}({\rm HL}) of each handlebody link HL{\rm HL} in Table 1, 𝖠k\mathsf{A}_{k} being the alternating group on kk letters, as well as an upper bound of the rank of π1(𝕊3HL¯)\pi_{1}(\overline{\mathbb{S}^{3}\setminus{\rm HL}}) computed by Appcontour [21].

The entry “split” refers to the split handlebody link HL\operatorname{HL} given by a trivial handlebody knot and an unknotted solid torus; the entry “fake 656_{5}” is the split handlebody link consisting of the handlebody knot HK41\operatorname{HK}4_{1}, Ishii-Kishimoto-Suzuki-Moriuchi’s 414_{1} in [10], and an unknotted solid torus; the entry “fake 6116_{11}” is 6116_{11} in Table 1 with one of the bottom crossings reversed, thus making the lower solid torus component split off.

Table 2. Kitano-Suzuki invariant for entries in Table 1.
handlebody link components ks𝖠4ks_{\mathsf{A}_{4}} ks𝖠5ks_{\mathsf{A}_{5}} rank
split trivial + unknot 178 3675 3
414_{1} trivial + unknot 114 600 3
515_{1} trivial + unknot 98 660 \leq 4
616_{1} trivial + unknot 90 600 3
626_{2} trivial + unknot 106 689 3
636_{3} trivial + unknot 90 469 3
646_{4} HK414_{1} + unknot 106 689 3
656_{5} HK414_{1} + unknot 210 \leq 4
fake 656_{5} HK414_{1} + unknot 274
666_{6} trivial + unknot 130 1380 3
676_{7} trivial + unknot 98 597 \leq 4
686_{8} trivial + unknot 114 1401 3
696_{9} trivial + 2 unknots 310 1841 4
6106_{10} trivial + 2 unknots 326 4
6116_{11} trivial + 2 unknots 486 5876 4
fake 6116_{11} trivial + 2 unknots 694
6126_{12} trivial + 2 unknots 502 5883 4
6136_{13} trivial + 2 unknots 822 4
6146_{14} trivial + 2 unknots 486 5876 4
6156_{15} trivial + 3 unknots 1242 5
Theorem 3.1 (Uniqueness).

Entries in Table 1 are all inequivalent.

Proof.

All entries in Table 1 except for the pairs (62,64)(6_{2},6_{4}) and (611,614)(6_{11},6_{14}) are distinguished by comparing their ks𝖠4ks_{\mathsf{A}_{4}} and ks𝖠5ks_{\mathsf{A}_{5}} invariants (shown in Table 2). On the other hand, 626_{2} and 646_{4} cannot be equivalent because the removal of the “unknot” component produces inequivalent handlebody knots: one being trivial, the other being HK41\operatorname{HK}4_{1}. Similarly, one can distinguish 6116_{11} and 6146_{14} by removing the solid torus component having a non-trivial linking number with the genus 22 handlebody component [16] in each of them, and observing that, for 6146_{14}, the resulting handlebody link is 414_{1}, whereas for 6116_{11}, we get the trivial split handlebody link. ∎

Remark 3.1.

The pairs (62,64)(6_{2},6_{4}) and (611,614)(6_{11},6_{14}) in fact have homeomorphic complements, and hence the fundamental group cannot discriminate. Fig. 3.1 and 3.2 illustrate how to obtain the complements of 626_{2} and 6116_{11} from 646_{4} and 6146_{14}, respectively, via 33-dimensional Dehn-twists (indicated by arrows).

Remark 3.2.

656_{5} viewed as a diagram of a spatial graph is the notorious figure eight puzzle devised by Steward Coffin [3]. The goal of the puzzle is to free the circle component from the knotted handcuff graph, i.e. to obtain the fake 656_{5} as a spatial graph. The impossibility of solving the puzzle then follows from computing ks𝖠4()ks_{\mathsf{A}_{4}}(\bullet) of 656_{5} and fake 656_{5} (Table 2). See [1], [15] for other proofs of this.

Refer to caption
\simeq
\simeq
\simeq
Figure 3.1. 626_{2} and 646_{4} have homeomorphic complements.
Refer to caption
\simeq
\simeq
Figure 3.2. 6116_{11} and 6146_{14} have homeomorphic complements.
Theorem 3.2 (Unsplittability).

Entries in Table 1 are all unsplittable.

Proof.

In most cases (51,61,62,63,64,67,69,610)(5_{1},6_{1},6_{2},6_{3},6_{4},6_{7},6_{9},6_{10}) unsplittability follows by computing the linking number [16] between pairs of components of a handlebody link. There are a few cases where the linking number vanishes, and we deal with these cases by computing the ks𝖠4ks_{\mathsf{A}_{4}}- and ks𝖠5ks_{\mathsf{A}_{5}}-invariants of the corresponding split handlebody links (Table 2).

If 656_{5} were split, then 656_{5} would be equivalent to the fake 656_{5} but this is not possible by Table 2. In the case of 414_{1}, 666_{6}, 686_{8}, if any of them were split, than it would be equivalent to “split” in Table 2, but that is not the case. A similar argument can be applied to 6116_{11} and 6146_{14}: if one of them were split, it would be equivalent to the fake 6116_{11}, in contradiction to Table 2. Lastly, we observe that 6126_{12} and 6136_{13} are non-split, for otherwise 414_{1} would be split. ∎

Below we recall the irreducibility test developed in [2]. A rr-generator link is a link whose knot group, the fundamental group of its complement, is of rank rr.

Lemma 3.3.

If the trivial knot is a factor of some factorization of a reducible (n,1)(n,1)-handlebody link HL{\rm HL}, then

12ks𝖠4(HL)+63n+24nand60ks𝖠5(HL)+144n+193n+225n.12\mid ks_{\mathsf{A}_{4}}({\rm HL})+6\cdot 3^{n}+2\cdot 4^{n}\quad\textbf{and}\quad 60\mid ks_{\mathsf{A}_{5}}({\rm HL})+14\cdot 4^{n}+19\cdot 3^{n}+22\cdot 5^{n}. (3.1)
Lemma 3.4.

If a 22-generator knot is factor of some factorization of a reducible (n,1)(n,1)-handlebody link HL{\rm HL}, then

12+24pks𝖠4(HL)+(6+16p)3n+(2+6p)4n,where p=0 or 1.12+24p\mid ks_{\mathsf{A}_{4}}({\rm HL})+(6+16p)\cdot 3^{n}+(2+6p)\cdot 4^{n},\hskip 3.00003pt\textbf{where $p=0$ or $1$}. (3.2)
Lemma 3.5.

If a 22-component, 22-generator link is a factor of some factorization of a reducible (n,1)(n,1)-handlebody link HL{\rm HL}, then

48+24pks𝖠4(HL)+(26+16p)3n1+(8+6p)4n1,where p=0,1,2,3 or 4.48+24p\mid ks_{\mathsf{A}_{4}}({\rm HL})+(26+16p)\cdot 3^{n-1}+(8+6p)\cdot 4^{n-1},\hskip 3.00003pt\textbf{where $p=0,1,2,3$ or $4$.} (3.3)

From the above lemmas, one derives the following irreducibility test (see [2] for more details), making use of the Grushko theorem [6].

Corollary 3.6 (Irreducibility test).

A 33-generator (2,1)(2,1)-handlebody link is irreducible if it fails to satisfy (3.1); a 44-generator (2,1)(2,1)-handlebody link is irreducible if it fails to satisfy (3.2); a 44-generator (3,1)(3,1)-handlebody link or a 55-generator (4,1)(4,1)-handlebody link is irreducible if it fails to satisfy (3.1) and (3.3).

Theorem 3.7 (Irreducibility).

Entries in Table1 are irreducible.

Proof.

Corollary 3.6, together with Table 2, shows that all but 696_{9}, 6126_{12} are irreducible. The irreducibility of 6126_{12} and 696_{9} follows from computing the linking number between each pair of components in each of them. Specifically, if 6126_{12} (resp. 696_{9}) is reducible, then either the trivial knot or a 22-generator 22-component link is a factor of some factorization of 6126_{12} (resp. 696_{9}). For 6126_{12}, the former case is not possible by (3.1); the latter impossible too, for otherwise the two solid torus components would have a trivial linking number. The same argument implies that 696_{9} cannot have a 22-generator 22-component link as a factor, and the trivial knot cannot be its factor either, since the homomorphism of integral homology

H1(V1)H1(V2)H1(𝕊3W¯)H_{1}(V_{1})\oplus H_{1}(V_{2})\rightarrow H_{1}(\overline{\mathbb{S}^{3}\setminus W})

is onto, where V1,V2V_{1},V_{2} are the solid torus components, and WW the genus 22 component. ∎

Remark 3.3.

The complement of 696_{9} is in fact \partial-reducible; one can see this by performing the twist operation, indicated by the arrow in Fig. 3.3, where it shows that its complement is homeomorphic to the complement of the order-11 connected sum (Definition 6.1) between two Hopf links (Fig. 3.3, right). In the connected case, no irreducible handlebody knot of genus 22 admits a \partial-reducible complement [24, Theorem 11], but when the genus is larger than 22, such handlebody knots exist [23, Example 5.55.5], [24, Section 55]. For a (n,1)(n,1)-handlebody link, we suspect that 696_{9} attains the lowest possible nn for such a phenomenon to happen.

Refer to caption
\simeq
\simeq
\simeq
\simeq
Refer to caption
\simeq
\simeq
Refer to caption
Figure 3.3. 696_{9} and fake 696_{9}.

4. Completeness

This section discusses completeness of Table 1. Recall first that a minimal diagram of a non-split, irreducible handlebody link has either 22- or 33-connectivity. IH-minimal diagrams with 33-connectivity are obtained from a software code, and IH-minimal diagrams with 22-connectivity are recovered by knot sum of spatial graphs.

4.1. Minimal diagrams with 3-connectivity

We consider plane graphs with two trivalent vertices and up to six quadrivalent vertices satisfying the properties:

  1. (1)

    each of them has edge-connectivity 33 as an abstract graph,

  2. (2)

    their double arcs can only connect two quadrivalent vertices as abstract graphs, and

  3. (3)

    their double arcs only form a “bigon” (a polygon with two sides; the case ‘i’ in Fig. 4.1) as plane graphs.

The reason of considering only double arcs connecting two quadrivalent vertices with a bigon configuration is because all the other cases lead to either non-R-minimal diagrams or diagrams with connectivity less than 33 (see Fig. 4.1, where “d, e, f, g, h” illustrate those double arcs connecting at least one trivalent vertex and “j, k, l” those connecting two quadrivalent vertices with a non-bigon configuration.)

Refer to caption
Refer to caption
Figure 4.1. Possible configurations for loops and double arcs.

We enumerate such plane graphs by the software code, and then recover diagrams from these plane graphs by adding an over- or under-crossing to each quadrivalent vertex. Note that the number (nn in Table 3) of components of the associated spatial graphs is independent of how over/under-crossings are chosen. To provide a glimpse of how the code works, we record in Table 3 the number of such plane graphs with cc quadrivalent vertices for each nn. To recover (n,1)(n,1)-handlebody links with n>1n>1 represented by IH-minimal diagrams with 33-connectivity, we need to consider the cases with n>1n>1 in Table 3. On the other hand, to produce (n,1)(n,1)-handlebody links represented by IH-minimal diagrams with 22-connectivity, spatial graphs admitting an R-minimal diagram with 33-connectivity up to 44 crossings are required; thus all cases with c4c\leq 4 have to be examined.

Table 3. Plane graphs given by the code.
cc n=1n=1 n=2n=2 n=3n=3 total
2 1 1
3 2 1 3
4 8 2 10
5 29 8 37
6 144 34 3 181

IH-minimal diagrams. We examine IH-minimality of diagrams produced by plane graphs with n2n\geq 2, and discard those obviously not IH-minimal. This excludes all diagrams produced by the code up to 55 crossings (Table 7), but for diagrams with 66 crossings, some diagrams are potentially IH-minimal: they represent handlebody links 616_{1}, 626_{2}, 636_{3} or 696_{9} in Table 1.

Lemma 4.1.

An IH-minimal diagram with 33-connectivity has crossing number c6c\geq 6, and if c=6c=6, it represents a handlebody link equivalent to 616_{1}, 626_{2}, 636_{3} or 696_{9}, up to mirror image.

Note that we cannot conclude diagrams of 61,62,636_{1},6_{2},6_{3} and 696_{9} in Table 1 are IH-minimal yet, as they might admit diagrams with 22-connectivity and fewer crossings.

R-minimal diagrams. To produce minimal diagrams with 22-connectivity up to 66 crossings, we need R-minimal diagrams up to 44 crossings. Inspecting R-minimality of diagrams produced by the code (Table 6) gives us the following lemma.

Lemma 4.2.

An R-minimal diagram with 33-connectivity and crossing number less than 55 represents one of the spatial graphs in Table 4, up to mirror image.

Table 4. Spatial graphs up to four crossings.
[Uncaptioned image]

G01\operatorname{G0_{1}} [Uncaptioned image]G21\operatorname{G2_{1}} [Uncaptioned image]G31\operatorname{G3_{1}} [Uncaptioned image]G41\operatorname{G4_{1}}
[Uncaptioned image]G42\operatorname{G4_{2}} [Uncaptioned image]G43\operatorname{G4_{3}} [Uncaptioned image]G44\operatorname{G4_{4}} [Uncaptioned image]G45\operatorname{G4_{5}}

4.2. Minimal diagrams with 2-connectivity

Recall a diagram DD with 22-connectivity can be decomposed into finitely many simpler tangle diagrams such that each associated diagram of spatial graphs has 33- or 44-connectivity (Fig. 1.1). Furthermore, if DD is R-minimal, each induced spatial graph diagram is also R-minimal. In particular, an IH-minimal diagram with 22-connectivity can be recovered by performing the order-2 vertex connected sum between spatial graphs admitting a minimal diagram with kk-connectivity, k>2k>2. Since we are interested in (n,1)(n,1)-handlebody links, only one summand is a spatial graph with two trivalent vertices, and the rest are links admitting a minimal diagram with 44-connectivity. Note that the simplest minimal diagram with 44-connectivity represents the Hopf link, and since we only consider minimal diagrams up to 66 crossings, there are at most three link summands. Thus, IH-minimal diagrams with 22-connectivity can be recovered by considering the seven possible configurations below:

  1. (1)

    G#L1G\#L_{1},

  2. (2)

    (G#L1)#L2G\#L_{1})\#L_{2},

  3. (3)

    G#(L1#L2)G\#(L_{1}\#L_{2}),

  4. (4)

    ((G#L1)#L2)#L3G\#L_{1})\#L_{2})\#L_{3},

  5. (5)

    (G#L1)#(L2#L3)G\#L_{1})\#(L_{2}\#L_{3}),

  6. (6)

    (G#(L1#L2))#L3G\#(L_{1}\#L_{2}))\#L_{3},

  7. (7)

    G#((L1#L2)#L3)G\#((L_{1}\#L_{2})\#L_{3}),

where GG is a spatial graph admitting a minimal diagram with 33-connectivity, and LiL_{i} is a link admitting a minimal diagram with 44-connectivity. In general it is not known if a minimal diagram with 44-connectivity always represents a prime link; it is the case, however, when the crossing number is less than 55. In fact, there are only four minimal diagrams with 44-connectivity up to 44 crossings, and they represent the Hopf link, the trefoil knot, the figure eight, and Solomon’s knot (L4a1), respectively.

Cases 44 through 77 are easily dealt with since GG must have no crossings, and hence it is the trivial theta curve G01\operatorname{G0_{1}}, and thus each LiL_{i} is necessarily the Hopf link, so the knot sums actually consist in ‘inserting a ring’ somewhere to the result of the previous knot sums. To produce irreducible handlebody links there is only one possibility, that is, adding one Hopf link to each of the three arcs of the trivial theta curve, and this gives us entry 6156_{15} in Table 1.

Cases 22 and 33 forces GG to have 22 crossings at most. It cannot have zero crossings (trivial theta curve), for otherwise, we could only get diagrams representing reducible handlebody links. Note also that there is no RR-minimal diagram with 11 crossing. Now, there is only one RR-minimal diagram with two crossings, this is, entry G212_{1} in Table 4 (Moriuchi’s 212_{1} in [18]).

Now, to add two Hopf links to it, i.e. to place two rings successively, we observe that one of them must be placed around the connecting arc of the handcuff graph by irreducibility. The second ring can be placed in three inequivalent ways, which yield entries 6126_{12}, 6136_{13} and 6146_{14} of Table 1.

Case 11 is more complicated, and we divided it into subcases based on the crossing number c:=c(G)c:=c(G). The case c=0c=0 is immediately excluded by irreducibility, so three possibilities remain: c{2,3,4}c\in\{2,3,4\}.

Subcase c(G)=2c(G)=2. GG is necessarily G212_{1} in Table 4, and LL cannot be a knot. Since the crossing number of LL cannot exceed 44, LL is either L2a1 (Hopf link) or L4a1 (Solomon’s knot). In either case, LL is to be added to the connecting arc of the handcuff graph to produce irreducible handlebody links, yielding entries 414_{1} and 686_{8} in Table 1.

Subcase c(G)=3c(G)=3. GG is necessarily G313_{1} (Moriuchi’s theta curve 313_{1} in [17]), so LL cannot be a knot, and hence is the Hopf link. There is only one place to add LL by irreducibility, and this leads to entry 515_{1} in Table 1.

Subcase c(G)=4c(G)=4. In this case, LL can only be the Hopf link; and there are five possible spatial graphs for GG, namely G414_{1}, G424_{2}, G434_{3}, G444_{4}, and G454_{5}:

  • For G414_{1} in Table 4 (Moriuchi’s non-prime handcuff graph 21#3212_{1}\#_{3}2_{1} [19]), there are two inequivalent ways to add LL which produce entries 646_{4} and 656_{5}.

  • For G424_{2} and G434_{3} in Table 4 (Moriuchi’s prime handcuff graph 414_{1} [18] and prime theta-curve 414_{1} [17], respectively), there is only one way to add the Hopf link in each case by irreducibility, and this gives 666_{6}, 676_{7} in Table 1, respectively.

  • For G444_{4} and G454_{5} in Table 4, again by irreducibility, there is only one way to add the Hopf link in each case, which gives us 6106_{10} and 6116_{11} in Table 1, respectively.

We summarize the discussion above in the following:

Lemma 4.3.

A non-split, irreducible handlebody link admitting an IH-minimal diagram with 22-connectivity and crossing number 6\leq 6 is equivalent, up to mirror image, to one of the following handlebody links:

41,52,64,65,66,67,68,610,611,612,613,614.4_{1},5_{2},6_{4},6_{5},6_{6},6_{7},6_{8},6_{10},6_{11},6_{12},6_{13},6_{14}. (4.1)

By Lemma 4.1, if any of (4.1) admits an IH-minimal diagram with 33-connectivity, it is equivalent to one of 61,62,636_{1},6_{2},6_{3}, 696_{9}, while by Lemma 4.1 if 61,62,636_{1},6_{2},6_{3} or 696_{9} admits an IH-minimal diagram with 22-connectivity and less than 66 crossings, it is equivalent to 414_{1} or 515_{1}, but neither situation can happen by Theorem 3.1.

Corollary 4.4.

Diagrams in Table 1 are all IH-minimal.

5. Chirality

5.1. Decomposable links

We consider order-22 connected sum (compare with Definition 6.1) for handlebody-link-disk pairs. A handlebod-link-disk pair is a handlebody link HL{\rm HL} with an oriented incompressible disk DHLD\subset{\rm HL}. A trivial knot with a meridian disk is considered as the trivial handlebody-link-disk pair.

Definition 5.1 (Order-2 connected sum).

Given two handlebody-link-disk pairs (HL1,D1)({\rm HL}_{1},D_{1}), (HL2,D2)({\rm HL}_{2},D_{2}) the order-2 connected sum (HL1,D1)#(HL2,D2)({\rm HL}_{1},D_{1})\#({\rm HL}_{2},D_{2}) is obtained as follows: first choose a 33-ball BiB_{i} of DiD_{i} in 𝕊3\mathbb{S}^{3} for each ii with Bi̊HLi\mathring{B_{i}}\cap{\rm HL}_{i} a tubular neighborhood N(Di)N(D_{i}) of DiD_{i} in HLi{\rm HL}_{i}; next, identify N(Di)¯\overline{N(D_{i})} with Di×[0,1]D_{i}\times[0,1] via the orientation of DiD_{i}. Then (HL1,D1)#(HL2,D2)({\rm HL}_{1},D_{1})\#({\rm HL}_{2},D_{2}) is given by removing Bi̊\mathring{B_{i}} and gluing the resulting manifolds via an orientation-reversing homeomorphism:

h:(𝕊3B1¯)(𝕊3B2¯)with h(D1×{j})=D2×{k}kj+1 mod 2.h:\partial(\overline{\mathbb{S}^{3}\setminus B_{1}})\rightarrow\partial(\overline{\mathbb{S}^{3}\setminus B_{2}})\quad\textbf{with $h(D_{1}\times\{j\})=D_{2}\times\{k\}$, $k\equiv j+1$ mod $2$}.

A non-split, irreducible handlebody link is decomposable if it is equivalent to an order-2 connected sum of non-trivial handlebody-link-disk pairs.

Refer to caption
B1B_{1}
B2B_{2}
HL1{\rm HL}_{1}
HL2{\rm HL}_{2}
D1×{1}D_{1}\times\{1\}

D1×{0}D_{1}\times\{0\}

D2×{0}D_{2}\times\{0\}

D2×{1}D_{2}\times\{1\}
Figure 5.1. Knot sum of handlebody-link-disk pairs

Decomposability is reflected in minimal diagrams in most examples here, thus we state the following conjecture.

Conjecture 5.1.

Minimal diagrams of a decomposable handlebody link have 22-connectivity.

Lemma 5.2.

For a non-split, irreducible handlebody link HL{\rm HL}, the following statements are equivalent:
• HL{\rm HL} is decomposable;
• there exists a 22-sphere 𝔖\mathfrak{S} in 𝕊3\mathbb{S}^{3} such that 𝔖\mathfrak{S} and HL{\rm HL} intersect at two incompressible disks in HL{\rm HL} and neither of BiHL¯\overline{B_{i}\setminus{\rm HL}}, i=1,2i=1,2, is a solid torus, where B1,B2B_{1},B_{2} are components of 𝕊3𝔖¯\overline{\mathbb{S}^{3}\setminus\mathfrak{S}};
• 𝕊3HL¯\overline{\mathbb{S}^{3}\setminus{\rm HL}} admits an incompressible, non-boundary parallel (or \partial-incompressible) annulus AA with A\partial A inessential in HL{\rm HL}.

Proof.

This follows from the definition of (\partial-) incompressibility. ∎

The annulus AA in Lemma 5.2 is called a decomposing annulus of HL{\rm HL}. Similarly, a decomposiing annulus AA of a handlebody-link-disk pair (HL,D)({\rm HL},D) is an incompressible, non-boundary parallel annulus AA with A\partial A inessential in HL{\rm HL} and disjoint from D\partial D; note that HL{\rm HL} in (HL,D)({\rm HL},D) could be reducible.

We now prove a unique decomposition theorem for handlebody links with no genus g>2g>2 component; a unique decomposition theorem for handlebody knots of arbitrary genus is given [14, Appendix BB] (see also [11]).

Theorem 5.3.

Given a non-split, irreducible handlebody link HL{\rm HL}, suppose no component of HL\operatorname{HL} has genus greater than 2, and A,AA,A^{\prime} are decomposing annuli inducing

HL(HL1,D1)#(HL2,D2),HL(HL1,D1)#(HL2,D2), respectively.{\rm HL}\simeq({\rm HL}_{1},D_{1})\#({\rm HL}_{2},D_{2}),\;{\rm HL}\simeq({\rm HL}_{1}^{\prime},D_{1}^{\prime})\#({\rm HL}_{2}^{\prime},D_{2}^{\prime}),\textbf{ respectively}. (5.1)

If (𝕊3HLi¯,Di),i=1,2(\overline{\mathbb{S}^{3}\setminus{\rm HL}_{i}},D_{i}),i=1,2, admits no decomposing annulus. Then A,AA,A^{\prime} are isotopic, in the sense that there exists an ambient isotopy ft:𝕊3𝕊3f_{t}:\mathbb{S}^{3}\rightarrow\mathbb{S}^{3} fixing HL\operatorname{HL} with f1(A)=Af_{1}(A)=A^{\prime}.

Proof.

Note first that if AA, AA^{\prime} are disjoint, then the assumption implies that they must be parallel and hence isotopic. Suppose AAA\cap A^{\prime}\neq\emptyset. Then we isotopy AA such that the number of components of AAA\cap A^{\prime} is minimized.

Claim: any circle or arc in AAA\cap A^{\prime} is essential in both AA and AA^{\prime}. Observe first that a circle component CC of AAA\cap A^{\prime} is either essential or inessential in both AA and AA^{\prime}, for assuming otherwise would contradict the incompressibility of A,AA,A^{\prime}. Suppose CC is inessential in both AA and AA^{\prime}, and is innermost in AA^{\prime}. Then CC bounds disks D,DD,D^{\prime} in A,AA,A^{\prime}, respectively. Since HL{\rm HL} is non-split, DDD\cup D^{\prime} bounds a 33-ball BB in 𝕊3HL¯\overline{\mathbb{S}^{3}\setminus{\rm HL}}. Isotopy DD across BB to DD^{\prime} induces a new annulus AA isotopic to the original one with AAA\cap A^{\prime} having less components, contradicting the minimality.

Similarly, if ll is an arc component of AAA\cap A^{\prime}, then it is either essential or inessential in both AA and AA^{\prime}, for assuming otherwise would contradict the \partial-incompressibility of A,AA,A^{\prime}. Suppose ll is inessential in both AA and AA^{\prime} and an innermost arc in AA^{\prime}. Then ll cuts off a disk DD^{\prime} from AA^{\prime} and a disk DD from AA. Let D^:=DD\hat{D}:=D\cup D^{\prime}. If D^\partial\hat{D} is inessential, then we can remove the intersection ll by isotopying AA across the ball bounded by D^\hat{D} and the disk bounded by D^\partial\hat{D} in HL\partial\operatorname{HL}, contradicting the minimality. If D^\partial\hat{D} is essential, then isotopying D^\hat{D}, we can disjoin D^\hat{D} from AA.

Now, it may be assumed that D1D_{1} is in a genus one component of HL1\operatorname{HL}_{1}, and hence D2D_{2} is in a component of HL2\operatorname{HL}_{2} with genus 2\leq 2. Since D^\partial\hat{D} is essential, D^\hat{D} has to be in a genus 22 component of HL2\operatorname{HL}_{2} containing D2D_{2}. Because D^D2=\partial\hat{D}\cap D_{2}=\emptyset, if D^\partial\hat{D} is essential on the boundary of the embedded solid torus (HL2N(D2))𝕊3\big{(}{\rm HL}_{2}\setminus N(D_{2})\big{)}\subset\mathbb{S}^{3}, D^\partial\hat{D} would be its longitude, where N(D2)N(D_{2}) is a tubular neighborhood of D2D_{2}, disjoint from D^\hat{D}, in HL2\operatorname{HL}_{2}. Particularly, HL2{\rm HL}_{2} and therefore HL{\rm HL} would be reducible, a contradiction. On the other hand, if D^\partial\hat{D} bounds a disk on (HL2N(D2))\partial\big{(}{\rm HL}_{2}\setminus N(D_{2})\big{)} that contains some components of N(D2)¯\partial\overline{N(D_{2})}, then D^\partial\hat{D} is inessential in HL2{\rm HL}_{2}, and hence in HL{\rm HL}, again contradicting the irreducibility of HL{\rm HL}.

The claim is proved, which also implies AAA\cap A^{\prime} contains either circles or arcs.

No essential circles. Suppose CC is an essential circle, and a closest circle to A\partial A^{\prime}. Let RR^{\prime} be the annulus cut off by CC from AA^{\prime} with AR=CA\cap R^{\prime}=C and RR an annulus cut off by CC from AA. We isotopy the incompressible annulus R^:=RR\hat{R}:=R\cup R^{\prime} away from AA. Since components of R^\partial\hat{R} are inessential in HL\operatorname{HL}, by the assumption, R^\hat{R} is either parallel to AA or boundary-parallel. In the former case, replacing AA with RR leads to a contradiction since RAR\cap A^{\prime} has less components than AAA\cap A^{\prime}. In the latter case, isotopying RR through the solid torus VV bounded by R^\hat{R} and the part of HL\partial{\rm HL} parallel to R^\hat{R} gives a new AA isotopic to the original one but with less components in AAA\cap A^{\prime}, contradicting the minimality.

No essential arcs. Suppose l1l_{1} is an essential arc. Then choose the essential arc l2l_{2} next to l1l_{1} in AA^{\prime} such that the disk DD^{\prime} cut off by l1,l2l_{1},l_{2} from AA^{\prime} has DA=l1l2D^{\prime}\cap A=l_{1}\cup l_{2} and is on the side of AA containing components of HL1\operatorname{HL}_{1}. Let DD be a disk cut off by l1,l2l_{1},l_{2} from AA. It may be assumed, by pushing DD away from AA, that DDD\cup D^{\prime} is disjoint from AA, and hence is on the genus 11 complement of HL1\operatorname{HL}_{1} containing D1D_{1}. Since A^:=DD\hat{A}:=D\cup D^{\prime} is disjoint from D1D_{1}, it is necessarily an annulus, for if it were a Möbious band, we would get a non-orientable surface embedded in 𝕊3\mathbb{S}^{3}. Furthermore, each component of A^\partial\hat{A} is necessarily inessential in HL1\operatorname{HL}_{1}, so it either bounds a meridian disk or is inessential in HL1\partial\operatorname{HL}_{1}. Note also it cannot be the case that one component of A^\partial\hat{A} is essential in HL1\partial\operatorname{HL}_{1} and the other inessential by the irreducibility of HL\operatorname{HL}. Suppose both components are inessential in HL1\partial\operatorname{HL}_{1}. Then A^\hat{A}, together with disks on HL1\partial\operatorname{HL}_{1} bounded by A^\partial\hat{A}, bounds a 33-ball, with which we can isotopy AA to remove the intersection l1,l2l_{1},l_{2}, contradicting the minimality. Suppose both components bound meridian disks in HL1\operatorname{HL}_{1}. Then A~=DcD\tilde{A}=D^{c}\cup D^{\prime} has A~\partial\tilde{A} inessential in HL1\partial\operatorname{HL}_{1}, where Dc=AD¯D^{c}=\overline{A\setminus D}. Thus we reduce it to the previous case. ∎

5.2. Chirality

We divide the proof of Theorem 1.2 into two lemmas.

Lemma 5.4.

All handlebody links except for 515_{1}, 636_{3}, 666_{6}, 676_{7}, 686_{8}, 6106_{10} in Table 1 are achiral.

Proof.

Except 626_{2}, equivalences between these handlebody links and their mirror images are easy to construct; an equivalence between 626_{2} and r626_{2} is depicted in Fig. 5.2

Refer to caption
\simeq
\simeq
\simeq
\simeq
Figure 5.2. 626_{2} and its mirror image.

Lemma 5.5.

515_{1}, 636_{3}, 666_{6}, 676_{7}, 686_{8}, 6106_{10} in Table 1 are chiral.

Proof.

Recall that, given a handlebody link HL{\rm HL}, if HL{\rm HL} and rHLr{\rm HL} are equivalent, then there is an orientation-reversing self-homeomorphism of 𝕊3\mathbb{S}^{3} sending HL{\rm HL} to HL{\rm HL}.

Observe that each of 51,66,68,6105_{1},6_{6},6_{8},6_{10} admits an obvious decomposing annulus satisfying conditions in Theorem 5.3; particularly the annulus in each of them is unique. Their chirality then follows readily from the fact that torus links are chiral.

To see chirality of 636_{3}, we observe that, given a (2,1)(2,1)-handlebody link HL{\rm HL}, any self-homeomorphism of 𝕊3\mathbb{S}^{3} preserving HL{\rm HL} sends the meridian mm and the preferred longitude ll of the circle component to m±1m^{\pm 1} and l±1l^{\pm 1}, respectively. In particular, any isomorphism on knot groups induced by such a homeomorphism sends the conjugacy class of mlm\cdot l in π1(𝕊3HL¯)\pi_{1}(\overline{\mathbb{S}^{3}\setminus{\rm HL}}) to the conjugacy class of mlm\cdot l, m1lm^{-1}\cdot l, ml1m\cdot l^{-1} or m1l1m^{-1}\cdot l^{-1}, depending on whether the homeomorphism is orientation-preserving.

Let NN be the number of conjugacy classes of homomorphisms from π1(𝕊3HL¯)\pi_{1}(\overline{\mathbb{S}^{3}\setminus{\rm HL}}) to a finite group 𝖦\mathsf{G} that sends mlm\cdot l (and hence m1l1m^{-1}\cdot l^{-1}) to 11, and rNrN the number of conjugacy classes of homomorphisms from π1(𝕊3HL¯)\pi_{1}(\overline{\mathbb{S}^{3}\setminus{\rm HL}}) to 𝖦\mathsf{G} that sends ml1m\cdot l^{-1} (and hence m1lm^{-1}\cdot l) to 11. Now, if HL{\rm HL} and its mirror image rHLr{\rm HL} are equivalent, then N=rNN=rN. This is however not the case with 636_{3}; when 𝖦=A5\mathsf{G}=A_{5}, we have (N,rN)=(77,111)(N,rN)=(77,111) as computed by [21].

Refer to caption
DD
(a) Pair (T,D)(T,D).
Refer to caption
α\alpha
Refer to caption
(b) Dual pair (K41,α)(\operatorname{K4_{1}},\alpha).
Refer to caption
SS
α\alpha
(c) Seifert surface SS.
Figure 5.3.
Refer to caption
link number =1=-1
link number =1=1
Figure 5.4. Hopf links with different orientations.

In the case of 676_{7} by Theorem 5.3, every self-homeomorphism ff of 𝕊3\mathbb{S}^{3} sending 676_{7} to itself induces a self-homeomorphism ff sending the handlebody-knot-disk pair (T,D)(T,D) in Fig. 3(a) to itself, or alternatively the (fattened) figure eight with an arc (K41,α)(\operatorname{K4_{1}},\alpha) in Fig. 3(b) to itself, where α\alpha is the dual one-simplex to DD.

Let SS be a minimal Seifert surface of the figure eight (Fig. 3(c)) containing the arc α\alpha. Then it can be further assumed that f(S)=Sf(S)=S, because the complement of the tubular neighborhood N(α)N(\alpha) of α\alpha in SS is a Seifert surface of a Hopf link, and up to ambient isotopy, the Hopf link admits two minimal Seifert surfaces, and only one of them can give us SS after gluing N(α)N(\alpha) back.

Since ff sends the complement SN(α)S\setminus N(\alpha) to Sf(N(α))S\setminus f\big{(}N(\alpha)\big{)}, if ff is orientation-reversing, then the two oriented Hopf links in Fig. 5.4 are ambient isotopic, but that is not possible by their linking numbers. ∎

6. Reducible handlebody links

In this section, we show that Table 5 classifies, up to ambient isotopy and mirror image, all non-split, reducible (n,1)(n,1)-handlebody links up to six crossings (Theorem 1.3). We begin by considering the order-11 connected sum for handlebody links.

6.1. Order-1 connected sum

A handlebody-link-component pair (HL,h)({\rm HL},h) is a handlebody link HL{\rm HL} with a selected component hh of HL{\rm HL}.

Definition 6.1 (Order-11 connected sum).

Let (HL1,h1)({\rm HL}_{1},h_{1}) and (HL2,h2)({\rm HL}_{2},h_{2}) be two handlebody-link-component pairs. Then their order-11 connected sum (HL1,h1)({\rm HL}_{1},h_{1})(HL2,h2)({\rm HL}_{2},h_{2}) is given by removing the interior of a 33-ball B1B_{1} (resp. B2B_{2}) in 𝕊3\mathbb{S}^{3} with B1HL1=B1h1B_{1}\cap\partial{\rm HL}_{1}=B_{1}\cap\partial h_{1} (resp. B2HL2=B2h2B_{2}\cap\partial{\rm HL}_{2}=B_{2}\cap\partial h_{2}) a 22-disk, and then gluing the resulting 33-manifolds 𝕊3B1¯\overline{\mathbb{S}^{3}\setminus B_{1}}, 𝕊3B2¯\overline{\mathbb{S}^{3}\setminus B_{2}} via an orientation-reversing homeomorphism f:(B1,(B1)h1)(B2,(B2)h2)f:(\partial B_{1},(\partial B_{1})\cap h_{1})\rightarrow(\partial B_{2},(\partial B_{2})\cap h_{2}). We use HL1{\rm HL}_{1}HL2{\rm HL}_{2} to denote the set of order-11 connected sums between HL1,HL2{\rm HL}_{1},{\rm HL}_{2} with all possible selected components.

Refer to caption
ff
B1B_{1}
B2B_{2}
Refer to caption
HL1{\rm HL}_{1}
HL2{\rm HL}_{2}
Refer to caption
h1h_{1}
h2h_{2}
(HL1,h1)(HL2,h2)\small({\rm HL}_{1},h_{1})\text{-{}-}({\rm HL}_{2},h_{2})
Refer to caption
Figure 6.1. Order-11 connected sum of (HL1,h1)({\rm HL}_{1},h_{1})(HL2,h2)({\rm HL}_{2},h_{2}).

The following generalizes the case of handlebody knots in [24, Theorem 22].

Theorem 6.1 (Uniqueness).

Given a non-split, reducible (n,1)(n,1)-handlebody link HL{\rm HL}, if HL(HL1,h1)(HL2,h2){\rm HL}\simeq({\rm HL}_{1},h_{1})\text{-{}-}({\rm HL}_{2},h_{2}), and HL(HL1,h1)(HL2,h2){\rm HL}\simeq({\rm HL}_{1}^{\prime},h_{1}^{\prime})\text{-{}-}({\rm HL}_{2}^{\prime},h_{2}^{\prime}), then (HLi,hi)(HLi,hi)({\rm HL}_{i},h_{i})\simeq({\rm HL}_{i}^{\prime},h_{i}^{\prime}), i=1,2i=1,2, up to reordering.

Proof.

Note first that, since HL{\rm HL} is non-split and reducible, HLi,HLi{\rm HL}_{i},{\rm HL}_{i}^{\prime}, i=1,2i=1,2, are non-split, and π1(𝕊3HL¯)\pi_{1}(\overline{\mathbb{S}^{3}\setminus{\rm HL}}) is a non-trivial free product 𝖦1𝖦2\mathsf{G}_{1}\ast\mathsf{G}_{2}, where 𝖦i\mathsf{G}_{i} is the knot group of HLi{\rm HL}_{i}, i=1,2i=1,2.

Let DD and DD^{\prime} be the separating disks in 𝕊3HL¯\overline{\mathbb{S}^{3}\setminus{\rm HL}} given by the factorizations HL(HL1,h1)(HL2,h2){\rm HL}\simeq({\rm HL}_{1},h_{1})\text{-{}-}({\rm HL}_{2},h_{2}) and HL(HL1,h1)(HL2,h2){\rm HL}\simeq({\rm HL}_{1}^{\prime},h_{1}^{\prime})\text{-{}-}({\rm HL}_{2}^{\prime},h_{2}^{\prime}), respectively. Suppose neither 𝖦1\mathsf{G}_{1} nor 𝖦2\mathsf{G}_{2} is isomorphic to \mathbb{Z}. Then, up to isotopy, DD=D^{\prime}\cap D=\emptyset by the innermost circle/arc argument.

Suppose one of 𝖦i,i=1,2\mathsf{G}_{i},i=1,2, say 𝖦1\mathsf{G}_{1}, is isomorphic to \mathbb{Z}, that is, HL1{\rm HL}_{1} is a trivial solid torus in 𝕊3\mathbb{S}^{3}. Then 𝖦2\mathsf{G}_{2} must be non-cyclic, since n>1n>1. Let DlD_{l} be the disk bounded by the longitude of HL1{\rm HL}_{1}, and isotopy D,DlD,D_{l} such that the number nn (resp. nln_{l}) of components of DDD^{\prime}\cap D (resp. DDlD^{\prime}\cap D_{l}) is minimized.

Claim: nl=0n_{l}=0. Note first that the minimality implies that DDlD^{\prime}\cap D_{l} contains no circle components. Now, consider a tubular neighborhood N(Dl)N(D_{l}) of DlD_{l} in 𝕊3HL¯\overline{\mathbb{S}^{3}\setminus\operatorname{HL}} small enough such that N(Dl)¯D=\overline{N(D_{l})}\cap D=\emptyset and N(Dl)¯D\overline{N(D_{l})}\cap D^{\prime} are some disks, each of which intersects Dl+D_{l}^{+} (resp. DlD_{l}^{-}) at exactly one arc on its boundary, where Dl±N(Dl)¯D_{l}^{\pm}\subset\partial\overline{N(D_{l})} are proper disks in 𝕊3HL¯\overline{\mathbb{S}^{3}\setminus\operatorname{HL}} parallel to DlD_{l}. The claim then follows once we have shown that N(Dl)N(D_{l}) can be isotopied away from DD^{\prime}.

To see this, we construct a labeled tree Υ\Upsilon from the complement of the intersection DDl±D^{\prime}\cap D_{l}^{\pm} in DD^{\prime}, where D±:=Dl+DlD^{\pm}:=D_{l}^{+}\cup D_{l}^{-}. Regard each component of D(DD±)D^{\prime}\setminus\big{(}D^{\prime}\cap D^{\pm}\big{)} as a node in Υ\Upsilon, and each arc in DDl±D^{\prime}\cap D_{l}^{\pm} as an edge in Υ\Upsilon connecting the two nodes representing the components of D(DD±)D^{\prime}\setminus\big{(}D^{\prime}\cap D^{\pm}\big{)} whose closures intersect at the arc. Since each arc in DD±D^{\prime}\cap D^{\pm} cuts DD^{\prime} into two, Υ\Upsilon is a tree. The first two figures from the left in Fig. 6.2 illustrate the construction.

Refer to caption
Figure 6.2. h(Dl)h(D_{l}) and Υ\Upsilon.

We label nodes and edges of Υ\Upsilon as follows: A node is labeled with II if the corresponding component of D(DD±)D^{\prime}\setminus\big{(}D^{\prime}\cap D^{\pm}\big{)} is inside N(Dl)N(D_{l}); otherwise the node is labeled with OO. An edge of Υ\Upsilon is labeled with ++ if the corresponding component of DDl±D^{\prime}\cap D^{\pm}_{l} is in Dl+D_{l}^{+}; otherwise, it is labeled with -.

The labeling on Υ\Upsilon has the following properties: (a) adjacent nodes have different labels; (b) a node with label II is bivalent, and the two adjacent edges are labeled with ++ and -, respectively, whereas a node labeled with OO could be multi-valent; (c) a one-valent node corresponds to an innermost arc in DD^{\prime}, and always has label OO.

Consider a maximal path ΓΥ\Gamma\subset\Upsilon starting from a one-valent node and with the property that adjacent edges of Γ\Gamma have different labels. Then the other end point of the path must be labeled with OO and it is either a one-valent node of Υ\Upsilon or a multi-valent node with all adjacent edges having the same label; the two figures from the right in Fig. 6.2 illustrate two possible maximal paths.

Without loss of generality, we may assume that the adjacent edge of the starting one-valent node of Γ\Gamma is labeled with ++. Denote the closure of the corresponding component of D(DD±)D^{\prime}\setminus\big{(}D^{\prime}\cap D^{\pm}\big{)} by DΓsD_{\Gamma}^{s}. Then DΓs\partial D_{\Gamma}^{s} bounds a disk TT on (HLN(Dl)¯)\partial({\rm HL}\cup\overline{N(D_{l})}). If TDl=T\cap D_{l}^{-}=\emptyset, then DΓsD=D_{\Gamma}^{s}\cap D=\emptyset and hence TD=T\cap D=\emptyset by the minimality of nn; however, if it were the case, one could reduce nln_{l} by isotopying DlD_{l} across the 33-ball bounded by DΓsD_{\Gamma}^{s} and TT. Hence TT must contain DlD_{l}^{-}. Since the adjacent edge of the starting node is labeled with ++, adjacent edges of the end node of Γ\Gamma in Υ\Upsilon are labeled with -. Denote by DΓeD_{\Gamma}^{e} the closure of the component corresponding to the end node. Then DΓe\partial D_{\Gamma}^{e} bounds a disk in (HLN(Dl)¯)\partial({\rm HL}\cup\overline{N(D_{l})}) that is contained in TT and has no intersection with Dl+D_{l}^{+}. Particularly, DΓeD=D_{\Gamma}^{e}\cap D=\emptyset by the minimality of nn, and there is an arc in DΓe\partial D_{\Gamma}^{e} cutting a disk D′′D^{\prime\prime} off TDl¯\overline{T\setminus D_{l}^{-}} with D̊′′D=D′′D=\mathring{D}^{\prime\prime}\cap D^{\prime}=D^{\prime\prime}\cap D=\emptyset, so one can slide N(Dl)N(D_{l}) over D′′D^{\prime\prime} (Fig. 6.3) to decrease nln_{l}, a contradiction.

Refer to caption
DD^{\prime}
TT
DlD_{l}
Refer to caption
TT
Refer to caption
DD^{\prime}
Refer to caption
DlD_{l}

D′′D^{\prime\prime}

Refer to caption
slide over D′′D^{\prime\prime}
Figure 6.3.

Consequently, such a path Γ\Gamma cannot exist, but this can happen only if Υ\Upsilon is empty. The claim is thus proved. It implies that HL1,HL1{\rm HL}_{1},{\rm HL}_{1}^{\prime} are trivial solid tori in 𝕊3\mathbb{S}^{3}, and HL2{\rm HL}_{2}, HL2{\rm HL}_{2}^{\prime} are equivalent to N(Dl)¯HL\overline{N(D_{l})}\cup{\rm HL}. ∎

6.2. Non-split, reducible handlebody links

Table 5. Reducible links with up to six crossings.
crossings c(L1)c(L_{1}) + c(L2)c(L_{2}) description |L1|L_{1}L2|L_{2}|
2 (1) 0 + 2 unknot – Hopf 1
4 (4) 0 + 4 unknot – L4a1 1
unknot – Hopf#Hopf 2
2 + 2 Hopf – Hopf 1
5 (4) 0 + 5 unknot – Whitehead 1
unknot – Trefoil#Hopf 2
3 + 2 trefoil – Hopf 1
6 (17) 0 + 6 unknot – L6aii, i=1,,5i=1,\dots,5 1
unknot – L6n1 1
unknot – L4a1#Hopf 3
unknot – (Hopf#Hopf)#Hopf 4
2 + 4 Hopf – L4a1 1
Hopf – Hopf#Hopf 2
4 + 2 K4a1 – Hopf 1

Table 5 lists all non-split, reducible (n,1)(n,1)-handlebody links obtained by performing order-11 connected sum on pairs of links (L1,L2)(L_{1},L_{2}) with crossing numbers (c1,c2)(c_{1},c_{2}) and c1+c26c_{1}+c_{2}\leq 6. Since n>1n>1, one of L1L_{1}, L2L_{2}, say L2L_{2}, is a link with more than one component. The number in parentheses indicates the total number of inequivalent reducible handlebody links of the given crossing number. By Theorem 6.1, isotopy types of L1L_{1} and L2L_{2} with selected components determine the isotopy type of the resulting handlebody link L1L_{1}L2L_{2}. Thus there are no duplicates in Table 5.

On the other hand, by Lemmas 4.1 and 4.3 and Theorem 3.7, minimal diagrams of non-split, reducible (n,1)(n,1)-handlebody links up to 66 crossings cannot have kk-connectivity, k>1k>1. This shows the completeness of Table 5.

In particular, every non-split, reducible (n,1)(n,1)-handlebody link in Table 5 admits a minimal diagram with 11-connectivity; thus we postulate the following conjecture.

Conjecture 6.2.

Every non-split, reducible handlebody link admits a minimal diagram with 11-connectivity.

Not every minimal diagram of a reducible handlebody link has 11-connectivity. By Theorem 6.1, Conjecture 6.2 implies the additivity of the crossing number (Conjecture 6.3), a reminiscence of a one-hundred years old problem in knot theory.

Conjecture 6.3.

If (HL1,h1)(HL2,h2)({\rm HL}_{1},h_{1})\text{-{}-}({\rm HL}_{2},h_{2}) is a (n,1)(n,1)-handlebody link, then

c((HL1,h1)(HL2,h2))=c(HL1)+c(HL2).c\big{(}({\rm HL}_{1},h_{1})\text{-{}-}({\rm HL}_{2},h_{2})\big{)}=c({\rm HL}_{1})+c({\rm HL}_{2}). (6.1)

Acknowledgements

The first author benefits from the support of the GNAMPA (Gruppo Nazionale per l’Analisi Matematica, la Probabilità e le loro Applicazioni) of INdAM (Istituto Nazionale di Alta Matematica). The second author benefits from the support of the Swiss National Science Foundation Professorship grant PP00P2_179110/1. The fourth author is supported by National Center of Theoretical Sciences.

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Appendix A Output of the code

A.1. Minimal diagrams from the code

The software code used in the paper exhaustively enumerates 33-edge-connected plane graphs with two trivalent vertices and qq quadrivalent vertices, 0<q60<q\leq 6, without double arcs that form a non-bigon. Note that the trivial theta curve is the only 33-edge-connected plane graph without quadrivalent vertices. The output of the code is examined and summarized in Table 3, while the detailed list is available on http://dmf.unicatt.it/paolini/handlebodylinks/, where each plane graph is described by its adjacent matrix together with a fixed ordering (clockwise or counterclockwise) of the edges adjacent to every vertex, as determined by the planar embedding.

A.1.1. Four crossings or less

In Table 6, we analyze the output of the code up to 44 quadrivalent vertices, where the column “quad. v.” lists the number of quadrivalent vertices and “ref. no.” the reference number of each plane graph in the output of the code. The column “induced diagrams” describes minimality of diagrams induced by each plane graph. Most induced diagrams are not minimal, and we record those that are and their isotopy types as special graphs or handlebody links, up to mirror image. Up to 44-crossings, no IH-minimal diagram with more than one component is found.

Table 6. Diagrams with up to 44 crossings.
quad. v. ref. no. induced diagrams
1 none none
2 #1 R-minimal; G212_{1} in Table 4; not IH-minimal
3 #1, not R-minimal
#2,#3 R-minimal; G323_{2} in Table 4; not IH-minimal
4 #1,#2 IH-minimal; G414_{1} in Table 4
#3 R-minimal; G323_{2} in Table 4; not IH-minimal
#4, #8 R-minimal; G424_{2} in Table 4; not IH-minimal
#5, #6, #7 R-minimal; G434_{3} in Table 4; not IH-minimal
#9 R-minimal; G444_{4} in Table 4; not IH-minimal
#10 R-minimal; G454_{5} in Table 4; not IH-minimal

A.1.2. Five and six crossing cases

Table 7. Diagrams with 55 crossings.
ref. no. description
#6, #11, #14 not R-minimal
#22, #26, #35 not IH-minimal
#36 not IH-minimal
#37 not R-minimal

In the 55 crossings case, the code finds 88 plane graphs with more than one components, out of a total of 3737 planar embeddings. Table 7 records the analysis for their induced diagrams; none of them gives IH-minimal diagrams. In the 66 crossing case, out of 181181 plane graphs, 3737 induces diagrams with more than one components. Table 8 records the minimality of their induced diagrams.

Table 8. Diagrams with 66 crossings.
ref. no. description
#5 616_{1} in Table 1
#15, #22, #34, #45, #54 not R-minimal
#56 616_{1} in Table 1
#60 626_{2} in Table 1
#70 636_{3} in Table 1
#73 not R-minimal
#83 626_{2} in Table 1
#84 616_{1} in Table 1
#86, #91, #92, #93 not R-minimal
#104, #105, #114, #117, #123 not IH-minimal
#134, #135, #137, #144 not IH-minimal
#161, #165 616_{1} in Table 1
#168, #169, #170,#171 not IH-minimal
#175 696_{9} in Table 1
#176 not IH-minimal
#177 not R-minimal
#179, #180 not IH-minimal
#181 696_{9} in Table 1

Fig. A.1 exemplifies how the analysis is done. Fig. 1(a) shows how the diagrams induced by Plane Graph #5 are equivalent to those by #161 and #165 in the case of 6 crossings, and Fig. 1(b) explains non-minimality of diagrams induced by Plane Graphs #168, #169, #170, #171.

Refer to caption
(a) Equivalent handlebody links from plane graphs.
Refer to caption
(b) Non-minimal diagrams.
Figure A.1.

A.1.3. Inequivalent planar embeddings

As a side remark, Fig. A.2 illustrates two examples of abstract graphs with inequivant planar embeddings: one with five quadrivalent vertices and the other with six. Note that the abstract graphs have 22-vertex-connectivity, consistent with the Whitney uniqueness theorem [25].

Refer to caption
#14\#14
#15\#15
(a) Five-quadrivalent-vertex graph.
Refer to caption
#91\#91
#90\#90
#89\#89
(b) Six-quadrivalent-vertex graph.
Figure A.2. Inequivalent planar embeddings.