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Alternating links on surfaces and volume bounds

Efstratia Kalfagianni  and  Jessica S. Purcell Department of Mathematics, Michigan State University, East Lansing, MI, 48824, USA [email protected] School of Mathematics, Monash University, VIC 3800, Australia [email protected]
Abstract.

Weakly generalised alternating knots are knots with an alternating projection onto a closed surface in a compact irreducible 3-manifold, and they share many hyperbolic geometric properties with usual alternating knots. For example, usual alternating knots have volume bounded above and below by the twist number of the alternating diagram due to Lackenby. Howie and Purcell showed that a similar lower bound holds for weakly generalised alternating knots. In this paper, we show that a generalisation of the upper volume bound does not hold, by producing a family of weakly generalised alternating knots in the 3-sphere with fixed twist number but unbounded volumes. As a corollary, generalised alternating knots can have arbitrarily small cusp density, in contrast with usual alternating knots whose cusp densities are bounded away from zero due to Lackenby and Purcell. On the other hand, we show that the twist number of a weakly generalised alternating projection does give two sided linear bounds on volume inside a thickened surface; we state some related open questions.

Key words and phrases:
hyperbolic knot, hyperbolic link, volume, slope length, cusp shape, Dehn filling
2010 Mathematics Subject Classification:
57M25, 57M27, 57M50

1. Introduction

Alternating knots have a diagram that alternates on the projection plane S2S^{2} in S3S^{3}. There have been several generalisations of alternating knots to project to other surfaces, such as toroidally alternating links of Adams [8], generalised alternating links of Ozawa [38], and FF-alternating links of Hayashi [29]. In his PhD thesis, Howie introduced a family of knots and links which also have diagrams that alternate on surfaces other than the usual projection plane, but without some of the restrictions of previous work. He called these knots and links weakly generalised alternating, to distinguish them from Ozawa’s links, and proved that the conditions he requires on the diagram are sufficient to guarantee that such knots are prime, nonsplit, with essential checkerboard surfaces [30]. See also [31, page 5] for some discussion of the differences between these links and others.

Recently, Howie and Purcell extended the definition of weakly generalised alternating links to include alternating links on surfaces embedded in any compact orientable 3-manifold, not just S3S^{3} [31]. They showed that such links have many geometric properties in common with usual alternating links in S3S^{3}. For example, Menasco was the first to give conditions on usual alternating links that guarantee they are hyperbolic [37]. These results were extended by several authors, such as by Adams [8], Hayashi [29], and Ozawa [38] for alternating links on surfaces other than S2S^{2} in S3S^{3}, and by Adams et al [1], and Champanerkar, Kofman, and Purcell [16] for alternating links in T2×T^{2}\times{\mathbb{R}}. In [31], Howie and Purcell give broad conditions that guarantee hyperbolicity in many additional cases, subsuming many of the previous results. They also consider geometry of surfaces embedded in such links, and link volumes.

In this paper, we focus again on volumes. The volume of a usual alternating link on S2S^{2} in S3S^{3} is bounded above and below by linear functions of the twist number of the link, due initially to work of Lackenby [35], with the lower bound improved by Agol, Storm, and W. Thurston [9], and the upper bound improved by Agol and D. Thurston [35, Appendix]. Note that the upper bound applies to any non-split link in S3S^{3}, not just alternating.

The problem of determining hyperbolic volumes of link complements has a long history. In addition to bounds on volumes of alternating links, there are known bounds or improved bounds on volumes of other families, such as highly twisted links [21, 40], 2-bridge links [28], links with certain symmetries [22], links with high amounts of generalised twisting [42, 23, 4], chain links [32], semi-adequate links [24], weaving links [15]. Considering upper bounds only, there are better upper bounds on volumes of twisted torus links [13], asymptotically sharp upper bounds in terms of crossing number for certain families [14], and bounds in terms of triple crossing number for others [2]. There are also improved upper bounds on volumes and simplicial volumes for links in S3S^{3} with diagrams with different features [3, 17, 18]. There remain many open questions on how the volume of a link behaves with respect to its diagrams and other invariants. A goal of research in knot and link volumes is to find relations of such behaviour for broader families of knots, or to characterise properties of diagrams that make such relations possible.

Weakly generalised alternating links form a much broader family of links than merely alternating links, but they have similarities with alternating links that allow extension of some of the tools effectively used in the usual alternating case. Thus it is a natural question to investigate their volumes.

In [31], Howie and Purcell show that a lower bound on volume, similar to that for alternating links, holds for a weakly generalised alternating link satisfying mild hypotheses. That is, they define the twist number on the projection surface and show there is a linear lower bound on volume in terms of the twist number. However, they do not discuss the question of the upper bound, motivating the following.

Question 1.1.

Let KK be a link with a weakly generalised alternating projection on an embedded surface FF in a compact, irreducible 3-manifold YY. Is there a linear function of the twist number on the projection surface FF that gives an upper bound on the volume of the link complement vol(YK)\operatorname{vol}(Y-K)?

In this paper, we address this question from different directions. Our first result is to show that the answer is no when Y=S3Y=S^{3}. Thus no linear function of twist number gives an upper bound on volumes for all weakly generalised alternating links.

Theorem 1.2.

There exists a family of weakly generalised alternating knots {Kn}n\{K_{n}\}_{n\in{\mathbb{N}}} in S3S^{3} with the following properties:

  • The projection surface FF of each KnK_{n} is a Heegaard surface of genus two.

  • The volume vol(Kn)\operatorname{vol}(K_{n})\to\infty as \to\infty.

  • The twist number of the diagram on FF is constant for all nn.

Theorem 1.2 is an immediate consequence of a more general theorem stated as Theorem 4.3 below.

One application of Theorem 1.2 is to cusp densities. Lackenby and Purcell [36] showed that usual alternating knots on S2S^{2} in S3S^{3} have cusp volumes bounded below in terms of the twist number of the knot, and that cusp densities of these knots are universally bounded away from zero. Recently, Bavier [10] generalised the lower bound on cusp volume to weakly generalised alternating knots satisfying mild hypotheses. However, Theorem 1.2 shows that a similar cusp density result cannot hold. Combining Theorem 1.2 with a result of Burton and Kalfagianni [12] gives the following.

Corollary 1.3.

There exist weakly generalised alternating knots with arbitrarily small cusp density.

The construction of the links in Theorem 1.2, or more precisely Theorem 4.3, uses heavily the fact that the links lie on a Heegaard surface FF of genus two in S3S^{3}. Recall that such a surface bounds a handlebody of genus two on both sides. Therefore FF is compressible, with several compressing discs, allowing us to twist the diagram without affecting the projection surface or the ambient manifold S3S^{3}. It is interesting to ask whether there exist linear upper bounds on volume in terms of twist number tF(π(K))t_{F}(\pi(K)) in the case that the projection surface FF is incompressible in YY. In fact, we show that there is an upper bound when Y=S×[1,1]Y=S\times[-1,1] and KK has a weakly generalised alternating projection onto F=S×{0}F=S\times\{0\}. More specifically, we show the following, where the lower bound is due to Howie and Purcell [31].

Theorem 1.4.

Let SS be a closed orientable surface of genus at least one, and let KK be a link that admits a twist-reduced weakly generalised alternating projection onto F=S×{0}F=S\times\{0\} in Y=S×[1,1]Y=S\times[-1,1], for which the complementary regions of Fπ(K)F-\pi(K) are discs. Then the interior of YKY-K admits a hyperbolic structure. If S=T2S=T^{2}, then we have

voct2tF(π(K))vol(YK)<10vtettF(π(K)),{{v_{\rm oct}}\over 2}\ t_{F}(\pi(K))\leq\operatorname{vol}(Y-K)<10\,{v_{\rm tet}}\cdot t_{F}(\pi(K)),

where vtet=1.01494{v_{\rm tet}}=1.01494\dots is the volume of a regular ideal tetrahedron and voct=3.66386{v_{\rm oct}}=3.66386\dots is the volume of a regular ideal octahedron.

If SS has genus at least two,

voct2(tF(π(K))3χ(F))vol(YK)<6vocttF(π(K)).{{v_{\rm oct}}\over 2}\ (t_{F}(\pi(K))-3\chi(F))\leq\operatorname{vol}(Y-K)<6\,{v_{\rm oct}}\cdot t_{F}(\pi(K)).

In Theorem 1.4, if SS is a torus then there is a unique hyperbolic structure on the interior of YKY-K, and the volume is the hyperbolic volume of this structure. However, if SS has genus at least two, there are many hyperbolic structures. By vol(YK)\operatorname{vol}(Y-K) we mean the volume of the unique hyperbolic structure on the interior of YKY-K for which the boundary components corresponding to S×{1}S\times\{-1\} and S×{1}S\times\{1\} are totally geodesic. This agrees with the definitions in [5, 31].

Theorem 1.4 has a somewhat surprising corollary, namely that there does exist an upper bound on the volume of a weakly generalised alternating link on a Heegaard torus FF in S3S^{3}; this is Corollary 5.1. (Recall that a Heegaard torus bounds a solid torus on each side.) Thus the fact that the family in Theorem 4.3 lies on Heegaard surfaces of genus at least two is necessary.

Theorem 1.4 should be compared to related work. Adams, Calderon, and Mayer [5] found upper bounds on volumes of an alternating knot KK on F=S×{0}F=S\times\{0\} in Y=S×[1,1]Y=S\times[-1,1] in terms of the crossing number cF(π(K))c_{F}(\pi(K)). For F=T2×{0}F=T^{2}\times\{0\} in Y=T2×Y=T^{2}\times{\mathbb{R}}, Champanerkar, Kofman and Purcell [16] found sharp upper bounds on volume in terms of the complementary regions in Fπ(K)F-\pi(K).

By contrasting Theorem 4.3 and Theorem 1.4, we are led to the following.

Question 1.5.

For which manifolds YY and which projection surfaces FF will a link with a weakly generalised alternating projection to FF in YY admit a linear upper bound on volume, or simplicial volume, in terms of twist number tF(π(K))t_{F}(\pi(K))? Will such a bound hold if FF is incompressible?

Acknowledgements. We thank Josh Howie for pointing out that Corollary 5.1 extends to lens spaces and toroidally alternating links. This work is based on research done while Kalfagianni was on sabbatical leave, supported by NSF grants DMS-1708249, DMS-2004155 and a grant from the Institute for Advanced Study (IAS) School of Mathematics. The authors thank the IAS for helping to support Purcell’s visit during this time. Purcell was also supported by the Australian Research Council, grant DP210103136.

2. Definitions

2.1. Weakly generalised alternating links

Throughout, we will take our projection surface FF to be an oriented, closed, connected surface embedded in a compact, irreducible, oriented 3-manifold YY, possibly with boundary. For the first part of the paper, namely through Section 4, YY will be S3S^{3}. In Section 5, Y=S×[1,1]Y=S\times[-1,1] and F=S×{0}F=S\times\{0\}. (Disconnected projection surfaces appear in [30, 31], but we will not consider that generality here.) Given a link KF×[0, 1]YK\subset F\times[0,\ 1]\subset Y in general position, the image of KK under a projection π:F×[0, 1]F\pi\colon F\times[0,\ 1]\to F, along with over–under crossing information at double points, is called a generalised link diagram, and is denoted by π(K)\pi(K). A generalised link diagram is said to be alternating if it can be oriented such that in each region of Fπ(K)F-\pi(K), crossings alternate over and under.

Definition 2.1.

A generalised diagram π(K)\pi(K) on FF is weakly prime if, for any embedded disc DFD\subset F that intersects π(K)\pi(K) exactly twice, we have:

  • If FS2F\neq S^{2}, then π(K)D\pi(K)\cap D is an arc without crossings.

  • If F=S2F=S^{2}, then π(K)\pi(K) has at least two crossings and either DD or the complement of DD intersects π(K)\pi(K) in an arc without crossings.

The diagram π(K)\pi(K) is called reduced alternating if it is alternating, weakly prime and each component of KK projects with at least one crossing on FF.

Howie has shown that the conditions on a reduced alternating diagram in S3S^{3} suffice to show that the link is nontrivial, nonsplit, and prime [30].

Definition 2.2.

We say that the representativity of a diagram π(K)F\pi(K)\subset F is at least ρ\rho, and we write r(π(K),F)ρr(\pi(K),F)\geq\rho, if the boundary of every compressing disc of FF intersects π(K)\pi(K) in at least ρ\rho points. If FF has no compressing disc, define r(π(K),F)=r(\pi(K),F)=\infty.

We say that the edge-representativity of π(K)\pi(K) is at least ρ\rho, and we write e(π(K),F)ρe(\pi(K),F)\geq\rho, if every essential curve on FF intersects π(K)\pi(K) at least ρ\rho times.

The terms representativity and edge-representativity for knots and links were introduced by Howie [30], motivated by terminology in topological graph theory; see for example the survey article [33]. Observe that the edge-representativity of a knot or link will always be at most its representativity.

The following definition originally appeared in Howie’s thesis [30] for links in S3S^{3}, and was generalised to compact irreducible 3-manifolds by Howie and Purcell [31].

Definition 2.3.

A diagram π(K)FY\pi(K)\subset F\subset Y is called weakly generalised alternating (WGA), if it is reduced alternating and:

  • the regions Fπ(K)F\smallsetminus\pi(K) admit a checkerboard coloring, and

  • the representativity satisfies r(π(K),F)4r(\pi(K),F)\geq 4.

A link KK that admits a WGA diagram is called weakly generalised alternating (WGA).

Howie and Purcell showed that the complement of a weakly generalised alternating link is nontrivial, irreducible, and boundary irreducible, again implying that the link is nonsplit in S3S^{3} [31, Corollary 3.16].

Definition 2.4.

Let π(K)\pi(K) be a WGA projection on a surface FF. A twist region of π(K)\pi(K) on FF is a portion of the underlying diagram graph of π(K)\pi(K) that is either:

  • a string of bigon regions arranged vertex to vertex that is maximal (i.e. not contained in a larger string of bigons of π(K)\pi(K)),

  • or a single vertex (i.e. crossing) adjacent to no bigons.

The twist number of π(K)\pi(K) on FF, denoted by tF(π(K))t_{F}(\pi(K)) is the number of twist regions of π(K)\pi(K).

Definition 2.5.

A WGA diagram π(K)F\pi(K)\subset F is called twist reduced if whenever there is a disc DFD\subset F such that D\partial D intersects π(K)\pi(K) exactly four times adjacent to two crossings, then one of the following holds:

  • DD contains a (possibly empty) sequence of bigons that is part of a larger twist region containing the two crossings, or

  • FDF\smallsetminus D contains a disc DD^{\prime}, with D\partial D^{\prime} intersecting π(K)\pi(K) four times adjacent to the same two crossings as D\partial D, and DD^{\prime} contains a string of bigons that forms a larger twist region containing the original two crossings. See Figure 1.

Refer to caption
Refer to caption
DD
\Rightarrow
DD
or
Refer to caption
DD^{\prime}
Refer to caption
Figure 1. A twist reduced diagram. Figure modified from [31].

Note that any WGA diagram can be modified to be twist reduced by performing a flype on a disc that does not contain bigons, moving two twist regions together. See also the discussion after Definitions 6.3 and 6.4 in [31]. Observe also that in the case that F=S2F=S^{2}, our definition of twist reduced agrees with that of Lackenby for usual alternating links [35]; compare Figure 1 with Figure 3 of that paper.

The following is a special case of a result of Howie and Purcell [31, Theorem 1.1].

Theorem 2.6 (Howie–Purcell).

Let π(K)\pi(K) be a weakly generalised alternating projection of a link KK on a closed surface FF of genus at least one in the 3-manifold Y=S3Y=S^{3}, or Y=S×[1,1]Y=S\times[-1,1] and F=S×{0}F=S\times\{0\} for a surface SS homeomorphic to FF. Suppose that YFY-F is atoroidal and that all the regions of Fπ(K)F-\pi(K) are discs. Finally, suppose that π(K)\pi(K) is twist-reduced and r(π(K),F)>4r(\pi(K),F)>4. Then the following hold.

  • YKY-K is hyperbolic.

  • The checkerboard surfaces of π(K)\pi(K) are essential in YKY-K.

  • The hyperbolic volume satisfies

    vol(YK)voct2(tF(π(K))χ(F)χ(Y)).\operatorname{vol}(Y-K)\geq{{v_{\rm oct}}\over 2}\ (t_{F}(\pi(K))-\chi(F)-\chi(\partial Y)).

In the theorem, the checkerboard surfaces of π(K)\pi(K) are obtained by taking the checkerboard colouring of Fπ(K)F-\pi(K) into white and shaded regions. Under the above hypothoses, these regions are coloured discs. Complete the union of the white discs into a spanning surface by joining two such dics by a twisted band when they are adjacent across a crossing of π(L)\pi(L). Similarly for shaded discs. The two surfaces that arise are the checkerboard surfaces for π(L)\pi(L).

We finish this subsection with the following result, which is a special case of results from [31] that we will need in later sections.

Theorem 2.7 (Howie–Purcell).

Let π(K)\pi(K) be a weakly generalised alternating projection of a knot KK on a closed surface FF of genus at least one in S3S^{3}. Suppose that S3FS^{3}-F is atoroidal and r(π(K),F)>4.r(\pi(K),F)>4. Then the following are true:

  1. (1)

    Suppose that TT is an essential torus in S3KS^{3}-K. Then the checkerboard surfaces of π(K)\pi(K) cut TT into annuli such that each boundary component of each of the annuli lies entirely in a single region of Fπ(K)F-\pi(K).

  2. (2)

    Suppose that S3KS^{3}-K contains an essential annulus. Then π(K)\pi(K) has only one twist region.

Proof.

Part (1) is a special case of Proposition 4.10 of [31]. We note that if S3KS^{3}-K contains an essential torus, then Fπ(K)F-\pi(K) must contain some regions that are not discs. Part (2) is a special case of Theorem 4.6 of [31]. ∎

2.2. Cusped manifolds

We will use the existence and non-existence of upper volume bounds to draw conclusions on cusp density of WGA knots. In this section, we review the necessary terminology.

Suppose M¯\overline{M} is a compact orientable 3-manifold with one component of M¯\partial\overline{M} a single torus, for example a knot complement, and suppose the interior MM¯M\subset\overline{M} admits a complete hyperbolic structure. We say MM is a cusped manifold. One end of MM is homeomorphic to T2×[1,)T^{2}\times[1,\infty). Denote this by CC. Under the covering map ρ:3M\rho\colon{\mathbb{H}}^{3}\to M, this end is geometrically realised as the image of a horoball Hi3H_{i}\subset{\mathbb{H}}^{3}, and the preimage ρ1(ρ(Hi))\rho^{-1}(\rho(H_{i})) is a collection of horoballs. By shrinking HiH_{i} if necessary, we may ensure that these horoballs have disjoint interiors in 3{\mathbb{H}}^{3}. For such a choice of HiH_{i}, ρ(Hi)=C\rho(H_{i})=C is said to be a horoball neighbourhood of the cusp CC, or horocusp in MM.

For a cusped manifold MM, a 1-parameter family of horoball neighbourhoods, parameterised by size of the neighbourhood, is obtained by expanding the horoball HiH_{i} while keeping the same limiting point on the sphere at infinity. Taking the preimage in 3{\mathbb{H}}^{3}, expanding HiH_{i} expands all horoballs in the collection ρ1(C)\rho^{-1}(C). We may expand until the collection of horoballs ρ1(C)\rho^{-1}(\cup C) become tangent, and cannot be expanded further while keeping their interiors disjoint. This is a maximal cusp. For the case here, in which MM has a single cusp, there is a unique choice of expansion, giving a unique maximal cusp.

Definition 2.8.

For a hyperbolic knot KK, with maximal cusp CC, the cusp volume of KK, denoted by CV(K){\rm CV}(K), is the volume of CC. This volume is half of the Euclidean area of C\partial C; see, for example, [45, Exercise 2.31].

The following is a result of Burton and Kalfagianni on cusp volumes, [12, Theorem 1.1].

Theorem 2.9 (Burton–Kalfagianni).

Let KK be a hyperbolic knot in S3S^{3} with maximal cusp CC and cusp volume CV(K)\operatorname{CV}(K). Suppose that S1S_{1} and S2S_{2} are essential spanning surfaces in S3KS^{3}-K and let i(S1,S2)0i(\partial S_{1},\partial S_{2})\neq 0 denote the minimal intersection number of S1,S2\partial S_{1},\partial S_{2} on the torus C\partial C. Then

CV(K)9(|χ(S1)|+|χ(S2)|)2i(S1,S2).\operatorname{CV}(K)\leq 9\ \dfrac{(|\chi(S_{1})|+|\chi(S_{2})|)^{2}}{i(\partial S_{1},\partial S_{2})}.

3. The construction of the knots

In this section, we will construct sequences of weakly generalised alternating knots in S3S^{3} that satisfy Theorem 4.3. In fact we will construct two distinct families of such knots. In the first family, which we will denote {Kn}n\{K_{n}\}_{n\in{\mathbb{N}}}, some components Fπ(Kn)F-\pi(K_{n}) will not be discs while in the second family, denoted {Kn}n\{K^{*}_{n}\}_{n\in{\mathbb{N}}}, all the complementary regions of the projections π(Kn)\pi(K^{*}_{n}) will be discs. For WGA knots in S3S^{3} with the latter property, Theorem 2.6 states that they are hyperbolic and their volume is bounded below by the quantity tF(π(Kn))χ(F)t_{F}(\pi(K^{*}_{n}))-\chi(F). For the knots {Kn}n\{K_{n}\}_{n\in{\mathbb{N}}}, we will use tools from [31] to show that their complements are hyperbolic; the requirement that all the regions of the WGA knot projections are discs is not necessary for the hyperbolicity claim of [31, Theorem 1.1].

3.1. The construction

Begin with a generalised projection surface that is a genus two surface FF embedded as a standard Heegaard surface in S3S^{3}, sketched as on the left of Figure 2. We construct two graphs on FF, which we will call the templates for the knots we construct.

The first template is obtained by running six parallel curves around each of the handles of the bounded handlebody cut off by FF in S3S^{3}. The curves lie in the shaded region shown in the middle of Figure 2. Three additional parallel curves encircle a disc in FF, and each of these three curves intersects each the six strands exactly four times. Together, these six plus three curves form a graph on FF, with 72 vertices in a grid-like pattern. This is shown in the middle of Figure 2. Notice that this graph can be embedded on the standard plane of projection in S3S^{3}. Alternatively, we view the standard plane of projection in S3S^{3} as cutting through the Heegaard surface FF, splitting it into a 3-punctured sphere above and a 3-punctured sphere below. This first template lies entirely on the 3-punctured sphere above the plane of projection.

Refer to caption
Figure 2. Left: a genus-2 Heegaard surface for S3S^{3}. Middle: the first template, giving a graph with 72 vertices and complementary regions all discs, except a single 3-punctured sphere region across the back. Right: the second template, giving a graph with 120 vertices and complementary regions all discs.

For the second template, add four additional curves to the first template. These curves are again parallel, disjoint from the six parallel strands running around the handles, and intersect each of the three other curves four times. Moreover, these curves run below the standard plane of projection for S3S^{3}, to run across the lower 3-punctured sphere of FF in eight arcs, in two parallel pairs. This is shown on the right of Figure 2. Each of the four curves adds twelve vertices to the graph on FF.

Make each template into an alternating link by assigning over/under crossing information to each vertex in an alternating fashion. Denote the link arising from the first template by K^\hat{K}, and the link arising from the secton by K^\hat{K}^{*}, with diagrams π(K^)\pi(\hat{K}) and π(K^)\pi(\hat{K}^{*}), respectively.

Lemma 3.1.

The diagrams π(K^)\pi(\hat{K}) and π(K^)\pi(\hat{K}^{*}) are checkerboard coloured and twist reduced.

Proof.

The best way to see both results is by inspection. The two diagrams are explicit. It is a somewhat soothing exercise to sketch the diagrams and colour the checkerboard surfaces by hand.

Alternatively, π(K^)\pi(\hat{K}) can be projected onto the usual plane of projection in S3S^{3}, giving an ordinary alternating link, which must be checkerboard coloured. Note that in this ordinary alternating link, the region on the outside has the same colouring as the two regions inside the loops that ran around the handles before the projection. Therefore the colouring transfers to the genus-2 surface, giving a consistent colouring on the single 3-punctured sphere region under the plane of projection. Adding four parallel curves to this, as in π(K^)\pi(\hat{K}^{*}), does not affect most faces. One can check, using the fact that there are exactly four new strands, that the faces that are changed can have colouring modified to give a unified checkerboard colouring of the diagram.

As for twist reduced, suppose there is a disc DD in either π(K^)\pi(\hat{K}) or π(K^)\pi(\hat{K}^{*}) with D\partial D meeting the diagram exactly four times, adajcent to exactly two crossings, as in Figure 1, left. Isotope D\partial D to run through the adjacent crossings. This splits D\partial D into two arcs between crossings, with each such arc lying in a single region of the diagram. Moreover, these two regions have the same colour. Thus such a disc will correspond to two regions of the same colour meeting at two distinct crossings. By inspection, most regions of the diagram are quads with four distinct regions meeting the four vertices (crossings) of the quad, so such a disc cannot run there. In the first template there is the 3-holed sphere region, but all similar coloured regions adjacent to the 3-holed sphere across crossings are distinct. Similarly in the second template there is another large disc region, but it meets only distinct regions at each of its crossings. Finally, in both templates there are exactly two bigon faces, and thus a disc meeting exactly two crossings encircling the bigon. This satisfies the definition of twist reduced. ∎

Next, replace each single crossing on FF in the link diagram π(K^)\pi(\hat{K}) and π(K^)\pi(\hat{K}^{*}) with an alternating twist region with a high number of crossings so that the link remains alternating on FF. Moreover, choose the twist region such that if the parallel strands of the template are oriented in the same direction, then the replacement preserves the orientation, as shown in Figure 3. Under this replacement, many bigon faces are added. Choose the parity of the number of crossings in each twist region so that the result is a diagram of a knot in both cases, rather than a link.

Refer to caption
Figure 3. Insert twist regions at each crossing to preserve an orientation.

Denote the knot arising from the first template by KK, and the knot arising from the second by KK^{*}.

Lemma 3.2.

The diagrams of the knots KK and KK^{*} are checkerboard coloured, twist reduced, and weakly prime.

Proof.

The diagrams of π(K^)\pi(\hat{K}) and π(K^)\pi(\hat{K}^{*}) are checkerboard coloured and twist reduced by Lemma 3.1. When adding bigons to these diagrams to form π(K)\pi(K) and π(K)\pi(K^{*}), the diagram remains checkerboard coloured and twist reduced, because new bigons are added only to existing twist regions.

Showing weakly prime requires a little more work. Consider the three closed curves of intersection of FF with the usual plane of projection in S3S^{3}; call them xx, yy, zz. These divide FF into two pairs of pants, or 3-punctured spheres, one above the plane of projection and one below. The entire knot KK lies above the plane of projection, and is disjoint from the 3-punctured sphere below the plane of projection. Most of the knot KK^{*} lies above the plane of projection, but eight unknotted arcs of the diagram lie below.

Now, suppose there is an embedded disc DD on FF whose boundary D\partial D intersects the diagram π(K)\pi(K) or π(K)\pi(K^{*}) in exactly two points. The boundary D\partial D must intersect each of the curves xx, yy, and zz in an even number of intersection points. If it intersects any of xx, yy, zz in more than zero points, then there exists an outermost arc of D\partial D co-bounding a disc with an arc of xx, yy, or zz, forming a bigon BB.

Suppose first that the boundary of the bigon B\partial B is disjoint from the knot diagram. Then we may use BB to isotope DD through xx, yy, or zz, to reduce the number of intersections with xx, yy, and zz. Repeat this a finite number of times to remove all bigons that are disjoint from the diagram.

Next suppose that the boundary of BB intersects the diagram. Again BB is a disc, so B\partial B intersects the knot diagram twice. Note that BB is embedded either above or below the plane of projection. If below, there are no crossings that BB could enclose, hence it bounds a single unknotted arc. If above, BB is a disc in a 3-punctured sphere containing a graph whose only vertices come from bigons replacing vertices in a grid of 72 or 120 points, with edges running from the outside of this grid. A grid is well known to form a prime diagram, with primeness unchanged by replacing a vertex with a twist region, so BB bounds a single unknotted arc of the diagram.

The boundary B\partial B is made up of two arcs, one on D\partial D and one on xx, yy, or zz. The diagram either intersects D\partial D twice, or D\partial D once and xx, yy, or zz once (if the diagram is that of KK^{*}). In the first case, the diagram intersects D\partial D twice in B\partial B; these must be the only intersections of D\partial D with the diagram. Hence since BB bounds an unknotted arc, so does DD. In the second case, use BB to isotope DD along the unknotted arc of the diagram, pushing it past xx, yy, or zz, and removing two intersections with these curves. After a finite number of steps, there are no bigons BB.

Then DD lies either completely above or completely below the plane of projection. As before, it follows that it meets the diagram in a single unknotted arc. Thus the diagram is weakly prime. ∎

Let uu, vv, and ww be the curves shown in Figure 4, which bound meridian discs in one of the handlebodies. Note they cut the surface FF into two 3-holed spheres. We may and will choose these curves to be disjoint from the vertices of our templates where the crossings of π(K)\pi(K) or π(K)\pi(K^{*}) occur.

Refer to captionuuvvwwRefer to caption
Figure 4. Shown are the curves uu, vv, and ww.
Lemma 3.3.

The edge-representativity e(π(K),F)e(\pi(K^{*}),F) is equal to four.

Proof.

The nontrivial curve xx on FF intersects π(K)\pi(K^{*}) four times, so edge-representativity is at most four. To show it is equal to four, we need to show that any other essential curve on FF intersects π(K)\pi(K^{*}) at least four times.

Let F\ell\subset F be an essential curve. Consider how \ell intersects the 3-holed spheres obtained by cutting FF along the curves uu, vv, and ww of Figure 4. If \ell is completely contained in one of the two 3-holed spheres, then the fact that \ell is essential on FF means it is parallel to one of the three boundary components. But in either 3-holed sphere, the graph of the template includes six strands of the diagram running between each pair of boundary components, separated by a large grid. A closed curve must intersect this graph at least six times; it follows that \ell intersects π(K)\pi(K^{*}) at least six times.

Next suppose \ell intersects both 3-holed spheres. Then it must meet each in a collection of arcs. If any of these arcs co-bounds a bigon with one of uu, vv, ww, then \ell can be simplified by isotoping through the bigon. Such an isotopy will at worst, only decrease the number of intersections of π(K)\pi(K^{*}) with \ell, so we assume now that there are no bigons.

Because \ell must alternate running between the two 3-holed spheres, it must have an essential arc on the left side. This is an essential arc on the 3-holed sphere, running from one boundary component to another, possibly the same component. If it runs from one boundary component to a distinct one, it is a seam. Otherwise it is a wave. Each seam must run through the four parallel strands appearing in KK^{*} and not KK. Each wave either runs through these strands, or through the six parallel strands or the grid portion of the graph appearing in both KK and KK^{*}. Thus in all cases, the arc meets π(K)\pi(K^{*}) at least four times. It follows that the edge-representativity is four. ∎

The next step of the construction is to modify the two diagrams of KK and KK^{*} by performing full (Dehn) twists of the handlebody H1H_{1} along the discs bounded by curves uu, vv, and ww, which we denote as twisting along uu, vv, and ww, for short. We will twist at least eight times along each curve. This adjusts the diagrams of KK, KK^{*} by adding at least eight full twists, forming new knots, which we denote by KTK_{T} and KTK_{T}^{*}.

Twisting along uu, vv, and ww gives a homeomorphism of the handlebody H1H_{1}. It restricts to a homeomorphism of FF, that is a product of powers of Dehn twist along the curves. In our case since we will twist at least eight times along each curve, the power of each Dehn twist will be at least eight.

Lemma 3.4.

Twisting along uu, vv, and ww yields knots KTK_{T} and KTK_{T}^{*} with diagrams that are alternating on FF, checkerboard coloured, twist reduced, and weakly prime. Further, the edge-representativity of π(KT)\pi(K_{T}^{*}) is four. Finally, the complementary regions of the diagram on FF have the same topological type as the complementary regions of π(K)\pi(K) or π(K)\pi(K^{*}) on FF. In particular, there is still one 3-punctured sphere region on Fπ(KT)F-\pi(K_{T}), and all other regions on Fπ(KT)F-\pi(K_{T}) and Fπ(KT)F-\pi(K_{T}^{*}) are discs.

Proof.

Twisting along any curve uu, vv or ww restricts to a power of a Dehn twist on FF; such a homeomorphism is the identity away from an annulus neighbourhood of the curve. That annulus intersects the knot diagram in six essential arcs running from one boundary component to the other. The arcs subdivide the annulus into six discs that are coloured in a checkerboard fashion. After twisting, the arcs run into the annulus, around its core some number of times, and then out, but no new crossings are added. Because the knot was alternating on FF before twisting, the new knot remains alternating on FF. The checkerboard coloured discs between arcs of the knot diagram are mapped to new discs, with checkerboard colouring preserved under twisting.

To see that the diagram is still weakly prime, suppose a disc DD on FF meets the diagram π(KT)\pi(K_{T}) or π(KT)\pi(K_{T}^{*}) twice transversally in edges. Apply the inverse Dehn twist to the picture. This preserves FF and takes diagram to π(K)\pi(K) or π(K)\pi(K^{*}), respectively, and takes DD to a disc now meeting π(K)\pi(K) or π(K)\pi(K^{*}) twice. Because π(K)\pi(K) and π(K)\pi(K^{*}) are weakly prime by Lemma 3.2, the disc must contain no crossings, both before and after homeomorphism, and π(KT)\pi(K_{T}) and π(KT)\pi(K_{T}^{*}) are weakly prime. A similar argument shows the diagram is still twist reduced after twisting.

As for edge-representativity, recall that by Lemma 3.3 any essential curve on FF meets π(K)\pi(K^{*}) at least four times. Since surface homeomorphisms map essential curves to essential curves and preserve intersection numbers of curves, it follows that any essential curve on FF meets π(KT)\pi(K_{T}^{*}) at least four times. Thus the edge-representativity of π(KT)\pi(K_{T}^{*}) is four. ∎

Recall that by construction the crossings of π(KT)\pi(K_{T}) or π(KT)\pi(K_{T}^{*}) are associated with the vertices of the corresponding templates. In particular we have arranged so that there are no crossings in the annuli where the Dehn twists along uu, vv, or ww are supported, and no crossings in the 3-punctured sphere below the plane of projection. All crossings of π(KT)\pi(K_{T}) and π(KT)\pi(K_{T}^{*}) on FF lie in one of two discs on FF, one on either side of the curve vv. We call these the alternating tangles of π(KT)\pi(K_{T}) or π(KT)\pi(K_{T}^{*}). They are illustrated for the template of KK^{*} in Figure 5, left, in the regions shaded in purple.

Refer to caption
Figure 5. Left: The alternating tangles of π(KT)\pi(K_{T}^{*}) are shaded in purple; π(KT)\pi(K_{T}) is similar. Right: Cutting H1H_{1} along discs bounded by uu, vv, ww.
Lemma 3.5.

Each of the knot diagrams π(KT)\pi(K_{T}) and π(KT)\pi(K_{T}^{*}) has representativity at least six.

Proof.

The surface FF divides S3S^{3} into two handlebodies. Denote the bounded handlebody by H1H_{1}, and the unbounded one (i.e. that contains infinity) by H2H_{2}. We must argue that every curve CC that bounds a compressing disc in either H1H_{1} or in H2H_{2} will intersect the diagram in at least six points. Observe first that uu, vv, and ww bound meridian disc of H1H_{1} meeting the diagram at least six times. We need to show a similar result for any choice of a curve CC bounding a compressing disc EE.

Suppose first that CC bounds a compressing disc for H1H_{1}. Note that the curves u,v,wu,v,w cut the surface FF into two pairs of pants, P1P_{1}, P2P_{2}, and the discs bounded by u,v,wu,v,w cut H1H_{1} into 3-balls. This is shown on the right of Figure 5. Isotope CC so that its intersection with uvwu\cup v\cup w is minimal on FF. By further isotopy we can arrange so that the disc EE bounded by CC intersects those bounded by u,v,wu,v,w in arcs (not simple closed curves). Now an arc of this intersection that is innermost on EE will define a wave on one of P1,P2P_{1},P_{2}. That is, it forms an essential arc on PiP_{i} with both of its boundary points on the same component of Pi\partial P_{i}. Such a wave will separate the two boundary components of PiP_{i} that is disjoint from. Thus it either runs through at least six parallel strands of the diagram, or it intersects the diagram in the alternating tangle. Within the alternating tangle, the number of intersection points must be at least six. Hence in either case, the wave will intersect the diagram in at least six points. This finishes the claim for H1H_{1}.

The proof for H2H_{2} is similar, only now cut H2H_{2} into balls bounded by pants along the plane of projection. This cuts FF into two pants, one above and one below the plane of projection, as shown in Figure 6.

Refer to caption
Figure 6. The form of the two pants obtained by cutting FF along the projection plane. The pants on the left lies above the plane of projection, and contains two alternating tangles plus a large number of parallel strands (at least six) following the arcs shown around those tangles (the dotted lines represent arcs in KK^{*} but not in KK). On the right is the pants below the plane of projection, with at least six strands running in the shaded regions shown.

Denote the boundary curves of the pants by xx, yy, and zz. A compressing disc EE for H2H_{2} can be isotoped to intersect xx, yy, and zz minimally, and to intersect the discs bounded by these curves only in arcs. Then an outermost arc of EE has boundary forming a wave. This wave separates boundary components, so again it either runs through the alternating tangle, meeting the knot diagram at least six times, or runs through a region with a high number of parallel strands, again meeting the knot diagram at least six times. ∎

The final step in the construction of the full sequence of knots for Theorem 4.3 is to twist along pairs of curves. Fix an integer m>0m>0. Add mm pairs of unknotted, unlinked components to the diagram C1,C2,,C2m1,C2mC_{1},C_{2},\dots,C_{2m-1},C_{2m} as shown in Figure 7.

Refer to caption
Refer to caption
C1C_{1}
C2C_{2}
C3C_{3}
C4C_{4}
C2mC_{2m}
C2m1C_{2m-1}
C2m2C_{2m-2}
C2m3C_{2m-3}
Figure 7. The curves to twist along.
Lemma 3.6.

Each curve CiC_{i} as above has linking number 0 with KTK_{T} or KTK_{T}^{*}.

Proof.

Consider the original template. Each curve CiC_{i} bounds a disc in S3S^{3} that is disjoint from all the curves of the original template, except meets each of the six parallel strands running over the handles of H1H_{1} exactly twice. Orient these strands in the same direction, as in the construction of KK and KK^{*}. Note each strand runs through the disc in one direction, then runs through again in the opposite direction, so each such strand has linking number zero with CiC_{i}. When we modified the template above to create the knot, in Subsection 3.1, we first inserted crossings at vertices. This did not affect orientation of strands through the CiC_{i}. We then added bigons to crossings on FF, chosen in such a way that the orientation of the six strands around handles is not affected, as in Figure 3. Finally we twisted along uu, vv, and ww. Again this had no effect on orientation of strands. Thus the linking number of KTK_{T} or KTK_{T}^{*} with any CiC_{i} is zero. ∎

For each CiC_{i}, select an integer ti7t_{i}\geq 7, and perform tit_{i} full twists along CiC_{i}. That is, drill CiC_{i} and perform 1/ti1/t_{i} Dehn filling. All choices of mm and all choices of integers ti7t_{i}\geq 7 give a countable collection of knots in S3S^{3}. Denote the sequence of knots obtained from twisting KTK_{T} by {Kn}\{K_{n}\}, nn\in{\mathbb{N}}. Denote the sequence obtained from KTK_{T}^{*} by {Kn}\{K_{n}^{*}\}, nn\in{\mathbb{N}}.

Lemma 3.7.

Any knot KTK_{T}, KTK_{T}^{*}, KnK_{n}, and KnK_{n}^{*} is a weakly generalized alternating knot (WGA), with representativity at least six and edge-representativity at least four. Furthermore, for every nn, the crossing number on FF, cF(π(Kn))c_{F}(\pi(K_{n})), is bounded, equal to cF(π(KT))=cF(π(K))c_{F}(\pi(K_{T}))=c_{F}(\pi(K)), and cF(π(Kn))=cF(π(KT))=cF(π(K))c_{F}(\pi(K_{n}^{*}))=c_{F}(\pi(K_{T}^{*}))=c_{F}(\pi(K^{*})). Similarly, the diagram is twist reduced, with bounded twist number on FF.

Finally, each KnK_{n} and KnK_{n}^{*} has linking number zero with each CiC_{i}.

Proof.

We have shown that π(KT)\pi(K_{T}) and π(KT)\pi(K_{T}^{*}) are alternating on FF, checkerboard coloured, weakly prime, and each component projects with at least one crossing by Lemma 3.4. The representativity of each is at least six by Lemma 3.5. Thus π(KT)\pi(K_{T}) and π(KT)\pi(K_{T}^{*}) are weakly generalized alternating. They are twist reduced with edge-representativity at least four by Lemma 3.4. We now show these properties for π(Kn)\pi(K_{n}) and π(Kn)\pi(K_{n}^{*}).

By choice, H1H_{1} is constructed as a 3-ball BB with with two unknotted and unlinked 2-handles. The co-cores of these 2-handles are meridians of H1H_{1}. The cores can be joined to a wedge of two circles on which H1H_{1} deformation retracts. Twisting along the curves CiC_{i} leaves the co-cores of the 2-handles of H1H_{1} fixed and inserts a 4-string pure braid to the wedge of two circles on which H1H_{1} retracts. The complement H2H_{2} is still a handlebody after twisting along the curves CiC_{i}. Indeed it is a complement of a 2-bridge link with an unknotting tunnel drilled out; see for example [34]. Thus after the twisting operation we still get a Heegaard splitting of S3S^{3}. We can isotope this Heegaard splitting to the original one by sliding around the discs on BB, on which the 2-handles of H1H_{1} are attached, until the 4-string braid on the spine is trivialized. This implies that the effect of twisting along the curves CiC_{i} is also achieved by a homeomorphism of S3S^{3} that preserves H1H_{1} and H2H_{2}. The restriction of the homeomorphism on FF fixes a set of meridian curves of H1H_{1} and restricts to a pure mapping class of the 4-holed sphere.

Since the property of bounding a meridian disc in H1H_{1} (resp. H2H_{2}) is preserved under homeomorphisms of H1H_{1} (resp. H2H_{2}) and intersection numbers of curves are preserved under homeomorphisms of FF, it follows that π(Kn)\pi(K_{n}) and π(Kn)\pi(K_{n}^{*}) have representativity at least six. Similarly, π(Kn)\pi(K_{n}) and π(Kn)\pi(K_{n}^{*}) remain alternating on FF after twisting along CiC_{i}, with the same number of crossings on FF as before, and the same twist number, and they remain checkerboard colored, twist reduced, and weakly prime on FF.

Thus the representativity of π(Kn)\pi(K_{n}) is identical to the representativity of π(K)\pi(K), hence it is at least six. Similarly for π(Kn)\pi(K_{n}^{*}). Similarly, edge-representativity is identical in both cases, hence it is at least four. ∎

Proposition 3.8.

Each WGA knot KTK_{T}, KTK_{T}^{*}, KnK_{n}, and KnK_{n}^{*} has hyperbolic complement in S3S^{3}.

Proof.

For KTK_{T}^{*} and KnK_{n}^{*}, the result follows immediately from Theorem 2.6: These knots are WGA in S3S^{3}, all regions on Fπ(KT)F-\pi(K_{T}^{*}) and Fπ(Kn)F-\pi(K_{n}^{*}) are discs, and the representativity is at least six, by Lemma 3.7. Thus by that theorem, these knots are hyperbolic.

The result is not quite as straightforward for KTK_{T} and KnK_{n}, because these knots have one region EE that is a 3-holed sphere, not a disc. For these knots, we show their complements are irreducible, boundary irreducible, anannular and atoroidal. For notational simplicity we will use S3JS^{3}-J to denote any of these manifolds.

We recall that  [31, Corollary 3.16] states that if π(L)\pi(L) is a reduced alternating link projection on a surface FF in a 3-manifold YY, them YLY-L is is irreducible and boundary irreducible. Hence the claim that S3JS^{3}-J is irreducible and boundary irreducible follows from the fact that the knot is WGA.

By construction, JJ has a WGA knot diagram π(J)\pi(J) that has more than one twist region. Thus part (2) of Theorem 2.7 implies that S3JS^{3}-J cannot contain an essential annulus.

Next we claim that S3JS^{3}-J is atoroidal. To prove it, suppose that TT is an essential torus in S3JS^{3}-J. By part (1) of Theorem 2.7, the checkerboard surfaces of π(J)\pi(J) cut TT into annuli A1,,AjA_{1},\dots,A_{j}, such that each boundary component of each AiA_{i} lies entirely in a single region of Fπ(J)F-\pi(J). Such a component cannot bound a disc (else use the fact that TT is incompressible and S3JS^{3}-J is irreducible to remove such an intersection), thus it must lie on a non-disc face of FJF-J. In our case there is only one non-disc face, namely the 3-holed sphere EE. The three components of E\partial E represent distinct free homotopy classes in H1H_{1}. Thus no two of these components can co-bound an annulus in H1H_{1}.

It follows that the components Ai\partial A_{i} must be parallel to a single component of E\partial E and parallel to each other. Then AiA_{i} is an annulus in a handlebody with parallel boundary components on the boundary of the handlebody. Thus AiA_{i} co-bounds a solid torus in the handlebody with an annulus on the boundary, and either AiA_{i} can be isotoped away from FF, or JJ lies inside that solid torus. However by Lemma 3.7, JJ has edge-representativity at least four. If JJ were contained in a solid torus parallel to an annulus on the boundary of H1H_{1}, then there would be an essential curve on H1\partial H_{1} disjoint from that annulus, implying the edge-representativity is zero. This is impossible. Thus JJ cannot lie entirely within a solid torus defined by AiA_{i}, and so we may isotope TT to avoid the intersections of Ai\partial A_{i}. Repeating this argument, all the intersections TFT\cap F can be eliminated by isotoping TT. But then TT is inessential in S3JS^{3}-J, a contradiction. ∎

4. Proofs of main results

This section completes the proofs of the volume result Theorem 4.3, and its consequence for cusp densities, Corollary 1.3. We will prove Theorem 4.3 by showing that the volumes of the knots {Kn}\{K_{n}\} or {Kn}\{K_{n}^{*}\} approach the volumes of another family {Lm}\{L_{m}\} with the property that vol(Lm)\operatorname{vol}(L_{m})\to\infty as mm\to\infty.

Let JJ be any knot in {Kn}n{Kn}n\{K_{n}\}_{n\in{\mathbb{N}}}\cup\{K^{*}_{n}\}_{n\in{\mathbb{N}}} and let Lm=J(i=1mC2i1C2i)L_{m}=J\cup(\bigcup_{i=1}^{m}C_{2i-1}\cup C_{2i}), where C1,C2,,C2m1,C2mC_{1},C_{2},\dots,C_{2m-1},C_{2m} are the curves shown in Figure 7 that produce JJ. We will show that the links LmL_{m} are hyperbolic. To do so, we use the following result of Gabai [27, Corollary 2.4].

Proposition 4.1 (Gabai).

Let MM be a Haken 3-manifold with toroidal boundary. If SS is a closed surface in MM that is not a boundary parallel torus, and such that SS is a Thurston norm minimizer in H2(M,M)H_{2}(M,\partial M), then SS remains norm minimizing in all but at most one of the 3-manifolds obtain by Dehn filling a along a single component of M\partial M. In particular, SS remains incompressible in all but at most one of the 3-manifolds obtain by Dehn filling along a single component of M\partial M. ∎

Recall the definition of the Thurston norm. If SS is a connected closed surface, then define χ(S)\chi_{-}(S) to be the negative of the Euler characteristic of SS, or χ(S)-\chi(S), if SS is not a 2-sphere. If SS is a 2-sphere, define χ(S)\chi_{-}(S) to be zero. If SS is not connected, then χ(S)\chi_{-}(S) is defined to be the sum of the complexities of the components of SS. Given SS as above, let cc denote the class of SS in H2(M,M)H_{2}(M,\partial M). The Thurston norm of cc is the minimum complexity χ(S)\chi_{-}(S) over all surfaces representing cc. A representative c=[S]c=[S] that realises the Thurston norm of cc is called a Thurston norm minimizer in its class.

Proposition 4.2.

The links {Lm}m\{L_{m}\}_{m\in{\mathbb{N}}} are hyperbolic.

Proof.

To see that S3LmS^{3}-L_{m} is boundary irreducible, note that since S3JS^{3}-J is irreducible and boundary irreducible (by Proposition 3.8), a boundary reducing disc DD in S3LmS^{3}-L_{m} must have its boundary on one of the boundary components corresponding to some CiC_{i}. Note that for ii odd, CiC_{i} does not bound a disc in the complement of JJ. For ii even, CiC_{i} bounds a disc in the complement of JJ, but this disc is pierced by Ci1C_{i-1}. Hence no such disc exists, and S3LmS^{3}-L_{m} is boundary irreducible.

Now suppose that S3(JC1)S^{3}-(J\cup C_{1}) is reducible. Then there is a sphere in S3(JC1)S^{3}-(J\cup C_{1}) that separates JJ from C1C_{1}. This is impossible since C1C_{1} is not homotopically trivial in S3JS^{3}-J. Similarly suppose S3(JC1C2)S^{3}-(J\cup C_{1}\cup C_{2}) is reducible. Then, since S3(JC1)S^{3}-(J\cup C_{1}) is irreducible, there must be a 2-sphere separating C2C_{2} from S3(JC1)S^{3}-(J\cup C_{1}). This is again impossible since C2C_{2} is not homotopically trivial in S3(JC1)S^{3}-(J\cup C_{1}). Continuing inductively we conclude that S3LmS^{3}-L_{m} is irreducible.

Next we argue that S3LmS^{3}-L_{m} is atoroidal. Suppose that there is an essential (i.e. incompressible and non-boundary parallel) torus T1T_{1} in M1=S3(JC1)M_{1}=S^{3}-(J\cup C_{1}). Consider the 3-manifolds obtained from M1M_{1} by 1/t11/t_{1} Dehn filling along C1C_{1}. Each of these 3-manifolds is the complement of a knot obtained from JJ by t1t_{1} full twists along the disc bounded by C1C_{1}. Hence for t1t_{1} large enough, each of these 3-manifolds is the complement of a WGA knot in one of the sequences {Kn}\{K_{n}\} or {Kn}\{K_{n}^{*}\}; see discussion before the statement of Lemma 3.7. Let us denote the corresponding knot by J(t1)J(t_{1}).

Since χ(T1)=0\chi(T_{1})=0, it is a Thurston norm minimizer in H2(M1,M1)H_{2}(M_{1},\partial M_{1}). Since M1M_{1} is the complement of a link, it is Haken. Applying Gabai’s Proposition 4.1 to the essential torus T1M1T_{1}\subset M_{1}, we conclude T1T_{1} remains incompressible in all the manifolds S3J(t1)S^{3}-J(t_{1}), for t1>>0t_{1}>>0. On the other hand S3J(t1)S^{3}-J(t_{1}) is the complement of a hyperbolic WGA knot by Proposition 3.8, and as such it cannot contain an essential torus. The only possibility is that T1T_{1} is boundary parallel in S3J(t1)S^{3}-J(t_{1}). This implies that C1C_{1} lies in a neighbourhood (N(J(t1)))×I\partial(N(J(t_{1})))\times I of the torus boundary of the knot complement, and thus it can be homotoped to lie on (N(J(t1)))\partial(N(J(t_{1}))).

By Lemma 3.7, C1C_{1} has linking number zero with J(t1)J(t_{1}). From the above discussion, it can be homotoped to lie on (N(J(t1)))\partial(N(J(t_{1}))). Hence C1C_{1} is either homotopically trivial on (N(J(t1)))\partial(N(J(t_{1}))) or homologous to a longitude of (N(J(t1)))\partial(N(J(t_{1}))). Suppose that C1C_{1} is homotopically trivial on (N(J(t1)))\partial(N(J(t_{1}))). Then C1C_{1} can be made to bound a disc in a 3-ball that is disjoint from N(J(t1))N(J(t_{1})) and from H1H_{1}. But this contradicts our choice of C1C_{1}. Next, suppose C1C_{1} homologous to a longitude of (N(J(t1)))\partial(N(J(t_{1}))), and thus a knot isotopic to J(t1)J(t_{1}) in S3S^{3}. However this is impossible since C1C_{1} bounds a disc in S3S^{3} and J(t1)J(t_{1}) does not. We conclude tha M1=S3(JC1)M_{1}=S^{3}-(J\cup C_{1}) is atoroidal.

Inductively, suppose 1<im1<i\leq m and (S3J)(j=1i1Cj)Ci(S^{3}-J)-(\bigcup_{j=1}^{i-1}C_{j})-C_{i} contains an essential torus. Again consider 1/ti1/t_{i} Dehn fillings on CiC_{i}, yielding a manifold (S3J(ti))(j=1i1Cj)(S^{3}-J(t_{i}))-(\bigcup_{j=1}^{i-1}C_{j}) where J(ti)J(t_{i}) is one of the WGA knots in {Kn}\{K_{n}\} or {Kn}\{K_{n}^{*}\}. For ti>>0t_{i}>>0, Gabai’s Proposition 4.1 again implies that the Dehn filling contains an incompressible torus. By induction, this must be boundary parallel in (S3J(ti))(j=1i1Cj)(S^{3}-J(t_{i}))-(\bigcup_{j=1}^{i-1}C_{j}). Thus C1C_{1} lies in a tubular neighbourhood of one of the link components CjC_{j} or J(ti)J(t_{i}). By linking number considerations as above, it cannot lie in a neighborhood of J(ti)J(t_{i}). By construction, it does not lie in a neighborhood of a component CjC_{j}. This contradiction proves the link is atoroidal.

Finally note that since no components of LnL_{n} co-bound an annulus in Nn=S3LnN_{n}=S^{3}-L_{n}, NnN_{n} contains no essential annuli and hence by Thurston’s hyperbolization theorem NnN_{n} is hyperbolic. ∎

We are now ready to prove the first main theorem, Theorem 4.3.

Theorem 4.3.

There exists a family of hyperbolic knots {Kn}n\{K_{n}\}_{n\in{\mathbb{N}}} in S3S^{3} with vol(Kn)\operatorname{vol}(K_{n}) approaching infinity as nn\to\infty, and such that KnK_{n} satisfy the following properties.

  • KnK_{n} has a weakly generalised alternating projection onto a Heegaard surface FF of genus two.

  • The representativity r(π(Kn),F)r(\pi(K_{n}),F) is at least six.

  • The crossing number cF(π(Kn))=cc_{F}(\pi(K_{n}))=c on FF is the same for all nn, and the twist number tF(π(Kn))=tt_{F}(\pi(K_{n}))=t on FF is the same for all nn.

  • Furthermore, we can take the knots KnK_{n} so that all the regions of the projections π(Kn)\pi(K_{n}) on FF are discs, and the edge-representativity is strictly greater than two. Alternatively, we can take the KnK_{n} to have a region that is not a disc.

In particular, neither the crossing number cF(π(K))c_{F}(\pi(K)) nor the number of twist regions tF(π(K))t_{F}(\pi(K)) on FF can give an upper bound on volume for a weakly generalised alternating link.

Observe that Theorem 4.3 immediately implies Theorem 1.2.

Proof of Theorem 4.3.

Fix V>0V>0. We will show there exist infinitely many WGA knots with volume strictly greater than VV. First, choose an integer m>0m>0 such that 2mv3>V2m\cdot v_{3}>V.

To produce the examples with disc regions and edge-representativity strictly greater than two, consider a knot JJ in {Kn}\{K_{n}^{*}\} obtained by Dehn filling 2m2m cusps of the 2m+12m+1 cusped manifold M=(S3KT)(i=1mC2i1C2i)M=(S^{3}-K_{T}^{*})-(\bigcup_{i=1}^{m}C_{2i-1}\cup C_{2i}). These have generalised diagrams whose complementary regions on FF are all discs. We argue that infinitely many such JJ have volume larger than VV. The link complement MM is hyperbolic by Proposition 4.2. Because it has 2m+12m+1 cusps, by Adams [7, Theorem 2.5],

vol(M)(2m+1)v3>(2m)v3>V.\operatorname{vol}(M)\geq(2m+1)\,v_{3}>(2m)\,v_{3}>V.

Recall that JJ is obtained by filling all the cusps of MM. For i=1,,2mi=1,\dots,2m, let tit_{i} be such that JJ is obtained by 1/ti1/t_{i} Dehn filling on the component CiC_{i}. Thurston’s hyperbolic Dehn filling theorem [46] implies that as the Dehn filling coefficients tit_{i} approach infinity, the volume of S3JS^{3}-J approaches vol(M)\operatorname{vol}(M) from below. In particular, for infinitely many such knots, the volume of the knot complement is strictly greater than 2mv3>V2m\cdot v_{3}>V, as required.

Finally, to produce examples with a complementary region on FF that is not a disc, run the same argument as above on knots in {Kn}\{K_{n}\}. ∎

This leads immediately to the proof of Corollary 1.3: that there exist weakly generalised hyperbolic knots in S3S^{3} with arbitrarily small cusp density.

Proof of Corollary 1.3.

Let {Kn}n\{K_{n}^{*}\}_{n\in{\mathbb{N}}} be the family of knots of Theorem 4.3 with disc regions. Let JJ be any knot in this family. By Theorem 2.6, the checkerboard surfaces S1S_{1}, S2S_{2} corresponding to the WGA knot π(J)\pi(J) are essential in S3JS^{3}-J. Let i(S1,S2)i(\partial S_{1},\partial S_{2}) denote the minimal intersection number of S1,S2\partial S_{1},\partial S_{2} on the torus boundary of the maximal cusp of KnK^{*}_{n}. So S1,S2S_{1},S_{2} are checkerboard surfaces of an alternating knot projection on a Heegaard surface FS3F\subset S^{3} and such that all the regions of the projection are discs. For such a situation the intersection number i(S1,S2)i(\partial S_{1},\partial S_{2}) and the quantity |χ(S1)|+|χ(S2)||\chi(S_{1})|+|\chi(S_{2})| are computed in the proof of [12, Theorem 1.2], where it its found that

|χ(S1)|+|χ(S2)|=cF(π(Kn))χ(F)=cF(π(Kn))+2andi(S1,S2)=2cF(π(Kn)).|\chi(S_{1})|+|\chi(S_{2})|=c_{F}(\pi(K_{n}^{*}))-\chi(F)=c_{F}(\pi(K_{n}^{*}))+2\ \ {\rm and}\ \ i(\partial S_{1},\partial S_{2})=2c_{F}(\pi(K_{n}^{*})).

By Theorem 2.9, we obtain

CV(Kn)92cF(π(Kn))(1+2cF(π(Kn))2.{\rm CV}(K_{n}^{*})\leq\dfrac{9}{2}\,c_{F}(\pi(K_{n}^{*}))\ \left(1+{{2}\over{c_{F}(\pi(K_{n}^{*})}}\right)^{2}.

By Lemma 3.7, cF(π(Kn))=cF(π(K))c_{F}(\pi(K_{n}^{*}))=c_{F}(\pi(K^{*})), and hence crossing number on FF is bounded independently of nn. Thus the cusp volume of KnK_{n}^{*} is uniformly bounded from above. On the other hand, by Theorem 4.3 we have vol(Kn)\operatorname{vol}(K_{n}^{*})\to\infty as nn\to\infty. Since the cusp density is by definition the quotient of CV(Kn){\rm CV}(K_{n}^{*}) by vol(Kn)\operatorname{vol}(K_{n}^{*}), the result follows. ∎

5. Links in thickened surfaces

The goal of this section is to prove Theorem 1.4 and Corollary 5.1.

Proof of Theorem 1.4.

Let Y=S×[1,1]Y=S\times[-1,1], F=S×{0}F=S\times\{0\}, and KK a WGA link as in the statement of the theorem. The fact that YKY-K is hyperbolic follows from Theorem 2.6: YFY-F is atoroidal, all regions are discs by hypothesis, and FF is incompressible, so the representativity is infinite. Thus the hypotheses of Theorem 2.6 hold and the link is hyperbolic. Recall that when the genus of SS is at least two, there are infinitely many hyperbolic structures, due to Thurston [47]. We choose the hyperbolic structure to be such that the higher genus boundary components are totally geodesic, as in [5, 31]; we refer to those papers for further details.

The lower volume bounds are given by Theorem 2.6: note Y\partial Y consists of two copies of FF, thus the terms χ(F)χ(Y)-\chi(F)-\chi(\partial Y) become 3χ(F)-3\chi(F). When FF is a torus, this is zero.

We obtain upper volume bounds similarly to [35, Appendix], by forming a fully augmented link; see also [44]. In particular, augment each twist region on FF by encircling it with a crossing circle, which bounds a 2-punctured disc punctured by KK. Untwist along each crossing circle: remove all pairs of crossings from each twist region. This is done by a homeomorphism of the complement of KK and the crossing circles. Let LL denote the resulting link. It consists of crossing circle components, bounding 3-punctured spheres meeting FF transversely, and components that came from KK. Components from KK are embedded on FF, except possibly in a neighbourhood of each crossing circle, where they may have a single crossing.

As in [35, Appendix], the fully augmented link on FF in S×[1,1]S\times[-1,1] can be decomposed into two geometric pieces, with totally geodesic boundary. The decomposition is obtained by cutting along two types of surfaces. The first surface consists of all the 2-punctured discs bounded by crossing circles. These are totally geodesic [6]. Shade them. They divide FLF-L into regions that will form the second surface. As in the case of a fully augmented link in S3S^{3}, a reflection through the projection surface takes YLY-L to a fully augmented link. The reflection reverses each single crossing, but following the reflection by a full-twist homeomorphism about the corresponding crossing circle takes the augmented link diagram back to itself. Thus there is an orientation-reversing self-homeomorphism of YLY-L. This fixes pointwise each of the regions of FLF-L away from crossing discs. It follows from Mostow–Prasad rigidity that these white regions glue to a white surface that is totally geodesic in YLY-L.

Cut along the white surface and the shaded discs. These give a decomposition of YLY-L into two isometric pieces, each homeomorpic to S×[0,1]S\times[0,1], with S×{0}S\times\{0\} marked by white and shaded faces meeting at ideal vertices. The shaded faces, coming from 2-punctured discs, are triangular. The white faces come from regions of FLF-L. White and shaded faces meet at right angles.

Consider first the case that S=T2S=T^{2}, a torus. Then T2×{1}T^{2}\times\{1\} is realised as a toroidal cusp of YLY-L. Cone each face on T2×{0}T^{2}\times\{0\} to the cusp T2×{1}T^{2}\times\{1\} to produce an ideal pyramid. The cone over a shaded face is a tetrahedron, one for each shaded face on each copy of T2×[0,1]T^{2}\times[0,1]. Two pyramids over a white face glue together to form a bipyramid; perform stellar subdivision of each white bipyramid. That is, subdivide a bipyramid into tetrahedra by removing the white face, taking an infinite geodesic dual to that face, and adding in triangles to divide the region into tetrahedra. If the white face has dd edges, the resulting subdivision gives dd tetrahedra; this subdivision is exactly as in [35, Appendix].

The count is also identical to that paper: Each crossing circle becomes four shaded triangles, giving rise to four tetrahedra. Each edge on T2×[0,1]T^{2}\times[0,1] that borders a white face gives rise to one tetrahedron, for both copies of T2×[0,1]T^{2}\times[0,1]. The subdivision gives three edges per crossing circle, each appearing twice on T2×[0,1]T^{2}\times[0,1]. This gives a total of six additional tetrahedra per crossing circle.

Thus we may subdivide the augmented link on the torus into 10tF(π(K))10\,t_{F}(\pi(K)) tetrahedra. The maximum volume of a tetrahedron is vtet=1.01494{v_{\rm tet}}=1.01494\dots. Thus

vol(YL)10vtettF(π(K)).\operatorname{vol}(Y-L)\leq 10\,{v_{\rm tet}}\cdot t_{F}(\pi(K)).

For the case Y=S×[1,1]Y=S\times[-1,1] with SS of higher genus, the argument is similar, but rather than coning to an ideal vertex at S×{1}S\times\{1\}, we cone white and shaded faces to ultra-ideal vertices coming from the totally geodesic surfaces at S×{1}S\times\{1\}, as in [5]. These are also referred to as hyperideal vertices, or truncated vertices, in the literature. Briefly, viewing 3{\mathbb{H}}^{3} in the Klein model, an ultra-ideal vertex lies outside the boundary at infinity. It defines a unique circle on the boundary at infinity, bounding a totally geodesic surface in 3{\mathbb{H}}^{3}, and we cut this off to form the truncated, ultra-ideal vertex. A generalised tetrahedron has at least one ultra-ideal vertex; topologically the tetrahedron is truncated at each ultra-ideal vertex. Geometrically, the totally geodesic faces of the tetrahedron meet a totally geodesic truncation face at right angles. See also [48] for a more detailed discussion.

In our situation, in the case of a white face, coning to an ultra-ideal vertex gives a truncated pyramid over the white face as a base. Gluing two white faces together produces a truncated bipyramid, with two ultra-ideal vertices, and an ideal dd-gon corresponding to the white face at the centre. As above, stellar subdivision divides these into generalised tetrahedra with two ideal vertices and two ultra-ideal vertices.

For each shaded face, take a truncated tetrahedron, with three ideal vertices and one ultra-ideal vertex. For ease of stating the bound, glue two shaded faces into a bipyramid over a triangle with two ultra-ideal vertices, and then perform stellar subdivision. Now each pair of shaded faces is divided into three generalised tetrahedra with two ideal vertices and two ultra-ideal vertices.

We count the number of generalised tetrahedra. Each crossing circle becomes four shaded triangles, giving rise to six generalised tetrahedra after gluing them in pairs and performing stellar subdivision. Each white face is bordered by some number of edges; each such edge gives rise to one generalised tetrahedron after stellation. Our decomposition into white and shaded faces above gives rise to three edges per crossing circle, each appearing twice as an edge of a white face. This gives a total of six additional generalised tetrahedra per crossing circle, or twelve total per crossing circle. (Observe that the count of tetrahedra meeting a white face is identical to the count above in the case of the torus, which is identical to the count in [35, Appendix]. The only difference is that now we count generalised tetrahedra.)

By Adams, Calderon, and Mayer [5, Corollary 3.4], the maximum volume of a generalised tetrahedron with two ideal vertices and two ultra-ideal vertices is voct/2{v_{\rm oct}}/2, where voct=3.66386{v_{\rm oct}}=3.66386\dots is the volume of a regular ideal octahedron. There are tF(π(K))t_{F}(\pi(K)) crossing circles. Thus

vol(YL)voct212tF(π(K))=6vocttF(π(K)).\operatorname{vol}(Y-L)\leq\frac{{v_{\rm oct}}}{2}\cdot 12\,t_{F}(\pi(K))=6{v_{\rm oct}}\,t_{F}(\pi(K)).

The link KK is obtained from LL by Dehn filling, and volume strictly decreases under Dehn filling [46]. Thus vol(YK)<vol(YL)\operatorname{vol}(Y-K)<\operatorname{vol}(Y-L), giving the result. ∎

Theorem 4.3 required a generalised projection surface of genus two. A similar construction could likely be made for a higher genus surface to give unbounded volume. However, the same result will not hold for a projection surface that is a torus. In particular, we now argue that there is an upper bound on volume in terms of tF(π(K))t_{F}(\pi(K)) for a WGA knot KK on a Heegaard torus in S3S^{3}, or indeed in any lens space.

Corollary 5.1.

Suppose KK is a link that has a weakly generalised alternating projection π(K)\pi(K) to a Heegaard torus FF in Y=S3Y=S^{3}, or in Y=L(p,q)Y=L(p,q) a lens space. Suppose that π(K)\pi(K) is twist reduced, the regions of Fπ(K)F-\pi(K) are discs, and the representativity satisfies r(π(K),F)>4r(\pi(K),F)>4. Then YKY-K is hyperbolic, and

voct2tF(π(K))vol(YK)<10vtettF(π(K)).{{v_{\rm oct}}\over 2}\ t_{F}(\pi(K))\leq\operatorname{vol}(Y-K)<10\,{v_{\rm tet}}\cdot t_{F}(\pi(K)).
Proof.

Set YY to be the manifold S3S^{3} or L(p,q)L(p,q). By Theorem 2.6, YKY-K is hyperbolic.

The Heegaard torus FF bounds solid tori V1V_{1} and V2V_{2} on either side. The core curves of the solid tori form a Hopf link in S3S^{3} if Y=S3Y=S^{3}, and some 2-component link if Y=L(p,q)Y=L(p,q). In the case of the Hopf link in S3S^{3}, drill the Hopf link from S3KS^{3}-K. The complement of the Hopf link in S3S^{3} is the manifold manifold T2×T^{2}\times{\mathbb{R}}. The surface FF is embedded as T2×{0}T^{2}\times\{0\}, and the knot KK lies on FF as a projection surface. Similarly, if YY is a lens space, then drilling the two core curves of the solid tori of YY gives the manifold T2×T^{2}\times{\mathbb{R}} with the surface FF embedded as T2×{0}T^{2}\times\{0\}, with the knot KK on FF.

Let XX be T2×T^{2}\times{\mathbb{R}} with (open) horoball neighbourhoods of the cusps at ±\pm\infty removed; thus XX is homeomorphic to T2×[1,1]T^{2}\times[-1,1]. The knot KK becomes a WGA knot on T2×{0}T^{2}\times\{0\} inside XX.

Now apply Theorem 1.4. That theorem implies that vol(XK)<10vtettF(π(K)).\operatorname{vol}(X-K)<10\,{v_{\rm tet}}\cdot t_{F}(\pi(K)).

Finally, the complement of the WGA knot YKY-K is obtained from XKX-K by Dehn filling along the 2-component link at the cores of the solid tori. Since volume strictly decreases under Dehn filling [46], vol(YK)<10vtettF(π(K))\operatorname{vol}(Y-K)<10\,{v_{\rm tet}}\,t_{F}(\pi(K)). ∎

Remark 5.2.

The proof of the upper bound of Corollary 5.1 uses restrictions on representativity only to guarantee the link complement is hyperbolic, using Theorem 2.6. In [8], Adams finds hyperbolicity conditions for alternating links on Heegaard tori in S3S^{3} and in lens spaces, which he calls toroidally alternating. Our upper volume bound will hold for toroidally alternating links that are hyperbolic, with no change to the proof.

Remark 5.3.

Dasbach and Lin [20] proved that the twist number of a reduced, twist reduced alternating link diagram on S2S^{2} is an invariant of the link, by relating the twist number to coefficients of the Jones polynomial. In [11], Bavier and Kalfagianni showed that the same is true for the links of Theorem 1.4 under the additional hypothesis that the edge-representativity of π(K)\pi(K) is at least four.

6. Further remarks

In this section we collect a few remarks, questions, and observations related to the main results.

6.1. A proof via generalised augmented links

Theorem 4.3 was proved by finding very straightforward lower bounds on volume using the number of cusps. In fact, better lower bounds on volume can be obtained for the knots {Kn}\{K_{n}\} with a 3-holed sphere region in the diagram. This is done by producing a generalised fully augmented link from the knot KnK_{n}. That is, in addition to adding components C1,,C2mC_{1},\dots,C_{2m}, add components u,v,wu,v,w from the construction as in Figure 4, and for each twist region on FF, add a crossing circle encircling that twist region, bounding a 3-punctured sphere. Generalised fully augmented links were considered in [41, 42, 43].

Similarly to the proof of Proposition 4.2, it can be shown that the fully augmented link is hyperbolic by ruling out essential spheres, discs, tori, and annuli; the arguments follow fairly similarly to those of [43]. Assuming hyperbolicity, [42, Theorem 4.2] implies the volume satisfies

vol(K)>0.64756(75+2m1).\operatorname{vol}(K)>0.64756\cdot(75+2m-1).

Here mm is the integer such that KK is obtained from KTK_{T} by twisting at least seven times along curves C1,,C2mC_{1},\dots,C_{2m}. The constant 0.647560.64756 can be improved as well as the amount of twisting increases, using a a theorem of Futer Kalfagianni and Purcell [21]. Indeed, this was our first approach to Theorem 4.3.

6.2. Lower bounds

The lower volume bounds from Howie and Purcell [31] on volumes of WGA knots in terms of twist regions on FF only apply to WGA knots with all complementary regions in Fπ(K)F-\pi(K) homeomorphic to discs. This does not apply to the knots {Kn}\{K_{n}\} with a 3-holed sphere region. It leads to the following natural question.

Question 6.1.

Suppose KK admits a weakly generalised alternating projection π(K)\pi(K) onto a generalised projection surface FF in S3S^{3}, or more generally in any compact orientable 3-manifold YY. Suppose the representativity is at least six, but at least one complementary region of π(K)\pi(K) on FF is not a disc. Suppose also that KK is hyperbolic. Is there a lower bound on the volume of the complement of KK in terms of the number of twist regions of KK on FF?

6.3. Turaev surfaces and adequate knots

In closing, we mention that all knots in S3S^{3} admit alternating checkerboard projections on certain Heegaard surfaces called Turaev surfaces; see [19]. In this setting an additional diagrammatic condition, called adequacy, also produces knots whose geometry shares many common properties with those of the usual alternating knots, such as volume bounds [24], topology and geometry of checkerboard surfaces [39, 25], and hyperbolicity [26]. However, the techniques of WGA links typically do not apply, because such diagrams have low representativity.

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