A table of -component handlebody links of genus up to six crossings
Abstract.
A handlebody link is a union of handlebodies of positive genus embedded in -space, which generalizes the notion of links in classical knot theory. In this paper, we consider handlebody links with one genus handlebody and solid tori, . 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 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 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 components having total genus . We call such a handlebody link an -handlebody link; it consists of exactly one genus handlebody and solid tori. The following theorems summarize the main results of the paper.
Theorem 1.1.
Table 1 enumerates all non-split111A handlebody link is split if there is a -sphere with separating into two parts., irreducible222A handlebody link is reducible if there is a -sphere in with an incompressible disk in . -handlebody links, up to ambient isotopy and mirror image, by their minimal diagrams, up to six crossings.
and in Table 1 are the only non-split, irreducible -handlebody links with four and five crossings, respectively. There are handlebody links with six crossings, among which have two components (), have three components (), and has four components (). As a side note, 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, in Table 1 is an irreducible handlebody link with a -irreducible complement; such phenomenon cannot happen when (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 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 -handlebody links up to six crossings (Section 4).
We first observe that the underlying plane graph of a diagram of a non-split, irreducible -handlebody link necessarily has edge connectivity equal to or ; for the sake of simplicity, such a diagram is said to have - or -connectivity, respectively. Diagrams with -connectivity up to six crossings are generated by a computer code, whereas to recover handlebody links represented by diagrams with -connectivity, we employ the knot sum—the order- vertex connected sum—of spatial graphs [17]. In more detail, a minimal diagram with -connectivity can be decomposed by decomposing circles333a circle that intersects at two different arcs. into simpler tangle diagrams, each of which induces a spatial graph that admits a minimal diagram with - or -connectivity, as illustrated in Fig. 1.1. This decomposition allows us to recover the handlebody link represented by by performing the knot sum between prime links and a spatial graph that admits a minimal diagram with -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 , , , , , 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- connected sum of handlebody-link-disk pairs (Definition 5.1).
Theorem 1.3.
Table 5 enumerates all non-split, reducible -handlebody links up to 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 -handlebody links in terms of order- 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 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 category; for the illustrative purposes, the drawings often appear smooth. In the case of -dimensional submanifolds in , the category is equivalent to the smooth category due to [4, Theorem ], [7, Theorems , ], [20, Theorem , , ].
![[Uncaptioned image]](https://cdn.awesomepapers.org/papers/5db12914-140d-44af-b213-d32b8c99495e/x5.png)
2. Preliminaries
2.1. Handlebody links and spatial graphs
Definition 2.1 (Embeddings in ).
A handlebody link (resp. a spatial graph ) 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 -sphere .
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 (resp. ) to denote the image of the embedding in . Let (resp. ) be the mirror image of (resp. ).
Definition 2.2 (Equivalence).
Two handlebody links , (resp. spatial graphs ) are equivalent if they are ambient isotopic; they are equivalent up to mirror image if (resp. ) is equivalent to or (resp. or ).
A regular neighborhood of a spatial graph defines a handlebody link, up to equivalence [22, ], and a spine of a handlebody link is a spatial graph with a regular neighborhood of [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 is a handlebody knot of genus , and is a set of disjoint incompressible disks in such that the complement of their tubular neighborhoods in consists of -balls, each of which has non-trivial intersection with exactly three components of . Such a disk system always exists.
Let disks be components of , and choose points in the interior of and a point in the interior of . Then, join to by a path for each ; this gives us a trivalent vertex. Repeat the construction for every , and then glue the together so that the vertices and are identified if they are in the same , for some . This way, we obtain a connected trivalent spine of with trivalent vertices. ∎
In general, a trivalent spine of a -component handlebody link of genus has trivalent vertices, and we call such a handlebody link a -handlebody link. This paper is primarily concerned with the case .
2.2. Diagrams
Let , and without loss of generality, it may be assumed handlebody links or spatial graphs are away from .
Definition 2.3 (Regular projection).
A regular projection of a spatial graph is a projection such that the set is finite with its cardinality for any , and no -simplex of the polygonal subset of is in the preimage of a double point, a double point being a point with .
As with the case of knots, up to ambient isotopy, every spatial graph admits a regular projection: the idea is to choose a vector neither parallel to a -simplex in the polygonal subset nor in a plane containing a -simplex and a -simplex or two -simplices; then isotopy slightly to remove those points with , where is the projection onto the plane normal to .
Definition 2.4 (Diagram of a spatial graph).
A diagram of a spatial graph is the image of a regular projection of 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 is a diagram of a spine of .
A diagram of (resp. ) 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 of a diagram of a handlebody link (resp. of a spatial graph ) is the number of crossings in . The crossing number of (resp. of ) is the minimum of the set
Definition 2.7 (Minimal diagram).
A minimal diagram of a handlebody link (resp. of a spatial graph ) is a diagram of (resp. ) with (resp. ).
Every multi-valent vertex in a minimal diagram can be replaced with some trivalent vertices by the inverse of the contraction move [9, Fig. ] without changing the crossing number, so for a handlebody link (resp. a spatial graph) there always exists a trivalent minimal diagram . 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 -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 trivalent vertices and quadrivalent vertices, then we can recover diagrams from it, up to mirror image. In particular, a -crossing -handlebody link can be recovered from one of these plane graphs. Therefore if one can enumerate all plane graphs with trivalent vertices and up to quadrivalent vertices, then one can find all -handlebody links up to crossings.
2.3. Moves
Definition 2.8 (Moves).
Note that spines of equivalent handlebody links might be inequivalent as spatial graphs; indeed, the following holds.
Theorem 2.2 ([12, Theorem ], [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 ]).
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.






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 -connectivity if its underlying plane graph has edge-connectivity .
Definition 2.11 (Split handlebody link).
A handlebody link is split if there exists a -sphere such that and both components of the complement have non-trivial intersection with .
Definition 2.12 (Reducible handlebody link).
A handlebody link is reducible if its complement admits a -sphere such that is an incompressible disk in ; otherwise it is irreducible.
Note that in Definition 2.12 factorizes into two handlebody links, each called a factor of the factorization of .
A diagram with -connectivity (resp. -connectivity) represents a split (resp. reducible) handlebody link, so only diagrams with connectivity greater than are of interest to us; on the other hand, the connectivity of a diagram of a -handlebody link with cannot exceed .
Now, we recall the order- vertex connected sum between spatial graphs [17], which is used to produce handlebody links represented by minimal diagrams with -connectivity. A trivial ball-arc pair of a spatial graph is a -ball with a trivial tangle in ; it is oriented if an orientation of is given.
Definition 2.13 (Knot sum).
Given two spatial graphs with oriented trivial ball-arc pairs of , respectively, their order- vertex connected sum is a spatial graph obtained by removing the interiors of and gluing the resulting manifolds and by an orientation-reserving homoemorphism
The notation denotes the set of order- vertex connected sums of given by all possible trivial ball-arc pairs.
Since an order- vertex connected sum depends only on the edges of intersecting with and their orientations, is a finite set.
3. Uniqueness, non-splittability, and irreducibility
Recall that, given a finite group , the Kitano-Suzuki invariant of a handlebody link is the number of conjugate classes of homomorphisms from to [13]. Table 2 lists the invariants and of each handlebody link in Table 1, being the alternating group on letters, as well as an upper bound of the rank of computed by Appcontour [21].
The entry “split” refers to the split handlebody link given by a trivial handlebody knot and an unknotted solid torus; the entry “fake ” is the split handlebody link consisting of the handlebody knot , Ishii-Kishimoto-Suzuki-Moriuchi’s in [10], and an unknotted solid torus; the entry “fake ” is in Table 1 with one of the bottom crossings reversed, thus making the lower solid torus component split off.
handlebody link | components | rank | ||
---|---|---|---|---|
split | trivial + unknot | 178 | 3675 | 3 |
trivial + unknot | 114 | 600 | 3 | |
trivial + unknot | 98 | 660 | 4 | |
trivial + unknot | 90 | 600 | 3 | |
trivial + unknot | 106 | 689 | 3 | |
trivial + unknot | 90 | 469 | 3 | |
HK + unknot | 106 | 689 | 3 | |
HK + unknot | 210 | 4 | ||
fake | HK + unknot | 274 | ||
trivial + unknot | 130 | 1380 | 3 | |
trivial + unknot | 98 | 597 | 4 | |
trivial + unknot | 114 | 1401 | 3 | |
trivial + 2 unknots | 310 | 1841 | 4 | |
trivial + 2 unknots | 326 | 4 | ||
trivial + 2 unknots | 486 | 5876 | 4 | |
fake | trivial + 2 unknots | 694 | ||
trivial + 2 unknots | 502 | 5883 | 4 | |
trivial + 2 unknots | 822 | 4 | ||
trivial + 2 unknots | 486 | 5876 | 4 | |
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 and are distinguished by comparing their and invariants (shown in Table 2). On the other hand, and cannot be equivalent because the removal of the “unknot” component produces inequivalent handlebody knots: one being trivial, the other being . Similarly, one can distinguish and by removing the solid torus component having a non-trivial linking number with the genus handlebody component [16] in each of them, and observing that, for , the resulting handlebody link is , whereas for , we get the trivial split handlebody link. ∎
Remark 3.1.
Remark 3.2.
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 as a spatial graph. The impossibility of solving the puzzle then follows from computing of and fake (Table 2). See [1], [15] for other proofs of this.
Theorem 3.2 (Unsplittability).
Entries in Table 1 are all unsplittable.
Proof.
In most cases 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 - and -invariants of the corresponding split handlebody links (Table 2).
If were split, then would be equivalent to the fake but this is not possible by Table 2. In the case of , , , 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 and : if one of them were split, it would be equivalent to the fake , in contradiction to Table 2. Lastly, we observe that and are non-split, for otherwise would be split. ∎
Below we recall the irreducibility test developed in [2]. A -generator link is a link whose knot group, the fundamental group of its complement, is of rank .
Lemma 3.3.
If the trivial knot is a factor of some factorization of a reducible -handlebody link , then
(3.1) |
Lemma 3.4.
If a -generator knot is factor of some factorization of a reducible -handlebody link , then
(3.2) |
Lemma 3.5.
If a -component, -generator link is a factor of some factorization of a reducible -handlebody link , then
(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).
Theorem 3.7 (Irreducibility).
Entries in Table1 are irreducible.
Proof.
Corollary 3.6, together with Table 2, shows that all but , are irreducible. The irreducibility of and follows from computing the linking number between each pair of components in each of them. Specifically, if (resp. ) is reducible, then either the trivial knot or a -generator -component link is a factor of some factorization of (resp. ). For , 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 cannot have a -generator -component link as a factor, and the trivial knot cannot be its factor either, since the homomorphism of integral homology
is onto, where are the solid torus components, and the genus component. ∎
Remark 3.3.
The complement of is in fact -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- connected sum (Definition 6.1) between two Hopf links (Fig. 3.3, right). In the connected case, no irreducible handlebody knot of genus admits a -reducible complement [24, Theorem ], but when the genus is larger than , such handlebody knots exist [23, Example ], [24, Section ]. For a -handlebody link, we suspect that attains the lowest possible for such a phenomenon to happen.
4. Completeness
This section discusses completeness of Table 1. Recall first that a minimal diagram of a non-split, irreducible handlebody link has either - or -connectivity. IH-minimal diagrams with -connectivity are obtained from a software code, and IH-minimal diagrams with -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)
each of them has edge-connectivity as an abstract graph,
-
(2)
their double arcs can only connect two quadrivalent vertices as abstract graphs, and
-
(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 (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.)


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 ( 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 quadrivalent vertices for each . To recover -handlebody links with represented by IH-minimal diagrams with -connectivity, we need to consider the cases with in Table 3. On the other hand, to produce -handlebody links represented by IH-minimal diagrams with -connectivity, spatial graphs admitting an R-minimal diagram with -connectivity up to crossings are required; thus all cases with have to be examined.
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 , and discard those obviously not IH-minimal. This excludes all diagrams produced by the code up to crossings (Table 7), but for diagrams with crossings, some diagrams are potentially IH-minimal: they represent handlebody links , , or in Table 1.
Lemma 4.1.
An IH-minimal diagram with -connectivity has crossing number , and if , it represents a handlebody link equivalent to , , or , up to mirror image.
Note that we cannot conclude diagrams of and in Table 1 are IH-minimal yet, as they might admit diagrams with -connectivity and fewer crossings.
R-minimal diagrams. To produce minimal diagrams with -connectivity up to crossings, we need R-minimal diagrams up to 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 -connectivity and crossing number less than represents one of the spatial graphs in Table 4, up to mirror image.
![[Uncaptioned image]](https://cdn.awesomepapers.org/papers/5db12914-140d-44af-b213-d32b8c99495e/x35.png)
4.2. Minimal diagrams with 2-connectivity
Recall a diagram with -connectivity can be decomposed into finitely many simpler tangle diagrams such that each associated diagram of spatial graphs has - or -connectivity (Fig. 1.1). Furthermore, if is R-minimal, each induced spatial graph diagram is also R-minimal. In particular, an IH-minimal diagram with -connectivity can be recovered by performing the order-2 vertex connected sum between spatial graphs admitting a minimal diagram with -connectivity, . Since we are interested in -handlebody links, only one summand is a spatial graph with two trivalent vertices, and the rest are links admitting a minimal diagram with -connectivity. Note that the simplest minimal diagram with -connectivity represents the Hopf link, and since we only consider minimal diagrams up to crossings, there are at most three link summands. Thus, IH-minimal diagrams with -connectivity can be recovered by considering the seven possible configurations below:
-
(1)
,
-
(2)
(,
-
(3)
,
-
(4)
((,
-
(5)
(,
-
(6)
(,
-
(7)
,
where is a spatial graph admitting a minimal diagram with -connectivity, and is a link admitting a minimal diagram with -connectivity. In general it is not known if a minimal diagram with -connectivity always represents a prime link; it is the case, however, when the crossing number is less than . In fact, there are only four minimal diagrams with -connectivity up to crossings, and they represent the Hopf link, the trefoil knot, the figure eight, and Solomon’s knot (L4a1), respectively.
Cases through are easily dealt with since must have no crossings, and hence it is the trivial theta curve , and thus each 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 in Table 1.
Cases and forces to have 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 -minimal diagram with crossing. Now, there is only one -minimal diagram with two crossings, this is, entry G in Table 4 (Moriuchi’s 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 , and of Table 1.
Case is more complicated, and we divided it into subcases based on the crossing number . The case is immediately excluded by irreducibility, so three possibilities remain: .
Subcase . is necessarily G in Table 4, and cannot be a knot. Since the crossing number of cannot exceed , is either L2a1 (Hopf link) or L4a1 (Solomon’s knot). In either case, is to be added to the connecting arc of the handcuff graph to produce irreducible handlebody links, yielding entries and in Table 1.
Subcase . is necessarily G (Moriuchi’s theta curve in [17]), so cannot be a knot, and hence is the Hopf link. There is only one place to add by irreducibility, and this leads to entry in Table 1.
Subcase . In this case, can only be the Hopf link; and there are five possible spatial graphs for , namely G, G, G, G, and G:
- •
- •
- •
We summarize the discussion above in the following:
Lemma 4.3.
A non-split, irreducible handlebody link admitting an IH-minimal diagram with -connectivity and crossing number is equivalent, up to mirror image, to one of the following handlebody links:
(4.1) |
By Lemma 4.1, if any of (4.1) admits an IH-minimal diagram with -connectivity, it is equivalent to one of , , while by Lemma 4.1 if or admits an IH-minimal diagram with -connectivity and less than crossings, it is equivalent to or , 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- connected sum (compare with Definition 6.1) for handlebody-link-disk pairs. A handlebod-link-disk pair is a handlebody link with an oriented incompressible disk . 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 , the order-2 connected sum is obtained as follows: first choose a -ball of in for each with a tubular neighborhood of in ; next, identify with via the orientation of . Then is given by removing and gluing the resulting manifolds via an orientation-reversing homeomorphism:
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.
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 -connectivity.
Lemma 5.2.
For a non-split, irreducible handlebody link ,
the following statements are equivalent:
• is decomposable;
• there exists a -sphere in
such that and intersect at two incompressible
disks in
and neither of , ,
is a solid torus,
where are components of ;
• admits an incompressible,
non-boundary parallel (or -incompressible)
annulus with inessential in .
Proof.
This follows from the definition of (-) incompressibility. ∎
The annulus in Lemma 5.2 is called a decomposing annulus of . Similarly, a decomposiing annulus of a handlebody-link-disk pair is an incompressible, non-boundary parallel annulus with inessential in and disjoint from ; note that in could be reducible.
We now prove a unique decomposition theorem for handlebody links with no genus component; a unique decomposition theorem for handlebody knots of arbitrary genus is given [14, Appendix ] (see also [11]).
Theorem 5.3.
Given a non-split, irreducible handlebody link , suppose no component of has genus greater than 2, and are decomposing annuli inducing
(5.1) |
If , admits no decomposing annulus. Then are isotopic, in the sense that there exists an ambient isotopy fixing with .
Proof.
Note first that if , are disjoint, then the assumption implies that they must be parallel and hence isotopic. Suppose . Then we isotopy such that the number of components of is minimized.
Claim: any circle or arc in is essential in both and . Observe first that a circle component of is either essential or inessential in both and , for assuming otherwise would contradict the incompressibility of . Suppose is inessential in both and , and is innermost in . Then bounds disks in , respectively. Since is non-split, bounds a -ball in . Isotopy across to induces a new annulus isotopic to the original one with having less components, contradicting the minimality.
Similarly, if is an arc component of , then it is either essential or inessential in both and , for assuming otherwise would contradict the -incompressibility of . Suppose is inessential in both and and an innermost arc in . Then cuts off a disk from and a disk from . Let . If is inessential, then we can remove the intersection by isotopying across the ball bounded by and the disk bounded by in , contradicting the minimality. If is essential, then isotopying , we can disjoin from .
Now, it may be assumed that is in a genus one component of , and hence is in a component of with genus . Since is essential, has to be in a genus component of containing . Because , if is essential on the boundary of the embedded solid torus , would be its longitude, where is a tubular neighborhood of , disjoint from , in . Particularly, and therefore would be reducible, a contradiction. On the other hand, if bounds a disk on that contains some components of , then is inessential in , and hence in , again contradicting the irreducibility of .
The claim is proved, which also implies contains either circles or arcs.
No essential circles. Suppose is an essential circle, and a closest circle to . Let be the annulus cut off by from with and an annulus cut off by from . We isotopy the incompressible annulus away from . Since components of are inessential in , by the assumption, is either parallel to or boundary-parallel. In the former case, replacing with leads to a contradiction since has less components than . In the latter case, isotopying through the solid torus bounded by and the part of parallel to gives a new isotopic to the original one but with less components in , contradicting the minimality.
No essential arcs. Suppose is an essential arc. Then choose the essential arc next to in such that the disk cut off by from has and is on the side of containing components of . Let be a disk cut off by from . It may be assumed, by pushing away from , that is disjoint from , and hence is on the genus complement of containing . Since is disjoint from , it is necessarily an annulus, for if it were a Möbious band, we would get a non-orientable surface embedded in . Furthermore, each component of is necessarily inessential in , so it either bounds a meridian disk or is inessential in . Note also it cannot be the case that one component of is essential in and the other inessential by the irreducibility of . Suppose both components are inessential in . Then , together with disks on bounded by , bounds a -ball, with which we can isotopy to remove the intersection , contradicting the minimality. Suppose both components bound meridian disks in . Then has inessential in , where . 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 , , , , , in Table 1 are achiral.
Proof.
Except , equivalences between these handlebody links and their mirror images are easy to construct; an equivalence between and r is depicted in Fig. 5.2

∎
Lemma 5.5.
, , , , , in Table 1 are chiral.
Proof.
Recall that, given a handlebody link , if and are equivalent, then there is an orientation-reversing self-homeomorphism of sending to .
Observe that each of 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 , we observe that, given a -handlebody link , any self-homeomorphism of preserving sends the meridian and the preferred longitude of the circle component to and , respectively. In particular, any isomorphism on knot groups induced by such a homeomorphism sends the conjugacy class of in to the conjugacy class of , , or , depending on whether the homeomorphism is orientation-preserving.
Let be the number of conjugacy classes of homomorphisms from to a finite group that sends (and hence ) to , and the number of conjugacy classes of homomorphisms from to that sends (and hence ) to . Now, if and its mirror image are equivalent, then . This is however not the case with ; when , we have as computed by [21].





link number |
link number |
In the case of by Theorem 5.3, every self-homeomorphism of sending to itself induces a self-homeomorphism sending the handlebody-knot-disk pair in Fig. 3(a) to itself, or alternatively the (fattened) figure eight with an arc in Fig. 3(b) to itself, where is the dual one-simplex to .
Let be a minimal Seifert surface of the figure eight (Fig. 3(c)) containing the arc . Then it can be further assumed that , because the complement of the tubular neighborhood of in 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 after gluing back.
Since sends the complement to , if 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 -handlebody links up to six crossings (Theorem 1.3). We begin by considering the order- connected sum for handlebody links.
6.1. Order-1 connected sum
A handlebody-link-component pair is a handlebody link with a selected component of .
Definition 6.1 (Order- connected sum).
Let and be two handlebody-link-component pairs. Then their order- connected sum – is given by removing the interior of a -ball (resp. ) in with (resp. ) a -disk, and then gluing the resulting -manifolds , via an orientation-reversing homeomorphism . We use – to denote the set of order- connected sums between with all possible selected components.




The following generalizes the case of handlebody knots in [24, Theorem ].
Theorem 6.1 (Uniqueness).
Given a non-split, reducible -handlebody link , if , and , then , , up to reordering.
Proof.
Note first that, since is non-split and reducible, , , are non-split, and is a non-trivial free product , where is the knot group of , .
Let and be the separating disks in given by the factorizations and , respectively. Suppose neither nor is isomorphic to . Then, up to isotopy, by the innermost circle/arc argument.
Suppose one of , say , is isomorphic to , that is, is a trivial solid torus in . Then must be non-cyclic, since . Let be the disk bounded by the longitude of , and isotopy such that the number (resp. ) of components of (resp. ) is minimized.
Claim: . Note first that the minimality implies that contains no circle components. Now, consider a tubular neighborhood of in small enough such that and are some disks, each of which intersects (resp. ) at exactly one arc on its boundary, where are proper disks in parallel to . The claim then follows once we have shown that can be isotopied away from .
To see this, we construct a labeled tree from the complement of the intersection in , where . Regard each component of as a node in , and each arc in as an edge in connecting the two nodes representing the components of whose closures intersect at the arc. Since each arc in cuts into two, is a tree. The first two figures from the left in Fig. 6.2 illustrate the construction.

We label nodes and edges of as follows: A node is labeled with if the corresponding component of is inside ; otherwise the node is labeled with . An edge of is labeled with if the corresponding component of is in ; otherwise, it is labeled with .
The labeling on has the following properties: (a) adjacent nodes have different labels; (b) a node with label is bivalent, and the two adjacent edges are labeled with and , respectively, whereas a node labeled with could be multi-valent; (c) a one-valent node corresponds to an innermost arc in , and always has label .
Consider a maximal path starting from a one-valent node and with the property that adjacent edges of have different labels. Then the other end point of the path must be labeled with and it is either a one-valent node of 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 is labeled with . Denote the closure of the corresponding component of by . Then bounds a disk on . If , then and hence by the minimality of ; however, if it were the case, one could reduce by isotopying across the -ball bounded by and . Hence must contain . Since the adjacent edge of the starting node is labeled with , adjacent edges of the end node of in are labeled with . Denote by the closure of the component corresponding to the end node. Then bounds a disk in that is contained in and has no intersection with . Particularly, by the minimality of , and there is an arc in cutting a disk off with , so one can slide over (Fig. 6.3) to decrease , a contradiction.





slide over |
Consequently, such a path cannot exist, but this can happen only if is empty. The claim is thus proved. It implies that are trivial solid tori in , and , are equivalent to . ∎
6.2. Non-split, reducible handlebody links
crossings | + | description | – |
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 – L6a, | 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 -handlebody links obtained by performing order- connected sum on pairs of links with crossing numbers and . Since , one of , , say , 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 and with selected components determine the isotopy type of the resulting handlebody link –. 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 -handlebody links up to crossings cannot have -connectivity, . This shows the completeness of Table 5.
In particular, every non-split, reducible -handlebody link in Table 5 admits a minimal diagram with -connectivity; thus we postulate the following conjecture.
Conjecture 6.2.
Every non-split, reducible handlebody link admits a minimal diagram with -connectivity.
Not every minimal diagram of a reducible handlebody link has -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 is a -handlebody link, then
(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 -edge-connected plane graphs with two trivalent vertices and quadrivalent vertices, , without double arcs that form a non-bigon. Note that the trivial theta curve is the only -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 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 -crossings, no IH-minimal diagram with more than one component is found.
quad. v. | ref. no. | induced diagrams |
---|---|---|
1 | none | none |
2 | #1 | R-minimal; G in Table 4; not IH-minimal |
3 | #1, | not R-minimal |
#2,#3 | R-minimal; G in Table 4; not IH-minimal | |
4 | #1,#2 | IH-minimal; G in Table 4 |
#3 | R-minimal; G in Table 4; not IH-minimal | |
#4, #8 | R-minimal; G in Table 4; not IH-minimal | |
#5, #6, #7 | R-minimal; G in Table 4; not IH-minimal | |
#9 | R-minimal; G in Table 4; not IH-minimal | |
#10 | R-minimal; G in Table 4; not IH-minimal |
A.1.2. Five and six crossing cases
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 crossings case, the code finds plane graphs with more than one components, out of a total of planar embeddings. Table 7 records the analysis for their induced diagrams; none of them gives IH-minimal diagrams. In the crossing case, out of plane graphs, induces diagrams with more than one components. Table 8 records the minimality of their induced diagrams.
ref. no. | description |
---|---|
#5 | in Table 1 |
#15, #22, #34, #45, #54 | not R-minimal |
#56 | in Table 1 |
#60 | in Table 1 |
#70 | in Table 1 |
#73 | not R-minimal |
#83 | in Table 1 |
#84 | 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 | in Table 1 |
#168, #169, #170,#171 | not IH-minimal |
#175 | in Table 1 |
#176 | not IH-minimal |
#177 | not R-minimal |
#179, #180 | not IH-minimal |
#181 | 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.


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 -vertex-connectivity, consistent with the Whitney uniqueness theorem [25].

