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Hyperbolic Manifolds Containing High Topological Index Surfaces

Marion Campisi San José State University
San Jose, CA 95192
marion.campisi@sjsu.edu
 and  Matt Rathbun California State University, Fullerton
Fullerton, CA 92831
mrathbun@fullerton.edu
Abstract.

If a graph is in bridge position in a 3-manifold so that the graph complement is irreducible and boundary irreducible, we generalize a result of Bachman and Schleimer to prove that the complexity of a surface properly embedded in the complement of the graph bounds the graph distance of the bridge surface. We use this result to construct, for any natural number nn, a hyperbolic manifold containing a surface of topological index nn.

1. Introduction

It has become increasingly common and useful to measure distances in complexes associated to surfaces between certain important sub-complexes associated with the surface embedded in a 3-manifold. These techniques provide a means to indicate the inherent complexity of links in a manifold, decomposing surfaces, or the manifold itself. In [4] Bachman defined the topological index of a surface as a topological analogue of the index of an unstable minimal surface. When the distance is small, the notion of topological index refines this distance, by looking at the homotopy type of a certain sub-complex.

In the same way that incompressible surfaces share important properties with strongly irreducible surfaces (distance >2>2) despite being compressible, the topological index provides a degree of measurement of how similar irreducible, but weakly reducible (distance =1=1) surfaces are to incompressible surfaces. In a series of papers [1, 2, 3], Bachman has shown that surfaces with a well-defined topological index in a 3-manifold can be put into a sort of normal form with respect to a trianglulation of the manifold, generalizing the ideas of normal form introduced by Kneser [18] and almost normal form introduced by Rubinstein [24], and mirroring results about geometrically minimal surfaces due to Colding and Minicozzi [10, 11, 12, 13, 14].

Lee [19] has shown that an irredubible manifold containing an incompressible surface contains topologically minimal surfaces of arbitrarily high genus, but has only shown that the topological index of such surfaces is at least two. In [6] Johnson and Bachman showed that surfaces of arbitrarily high index exist. These surfaces are the lifts of Heegaard surfaces in an n-fold cover of a manifold obtained by gluing together boundary components of the complement of a link in S3S^{3}. A by-product of their construction is that the resulting manifolds are toroidal.

This leaves open the question of whether the much more ubiquitous class of hyperbolic manifolds can also contain high topological index surfaces. Here we construct certain hyperbolic manifolds containing such surfaces. We generalize the construction in [6] by gluing along the boundary components of the complement of a graph in S3S^{3} to show:

Theorem 1.1.

There is a closed 3-manifold M1M^{1}, with an index 1 Heegaard surface SS, such that for each nn, the lift of SS to some nn-fold cover MnM^{n} of M1M^{1} has topological index nn. Moreover, MnM^{n} is hyperbolic for all nn.

In order to guarantee the hyperbolicity of MnM^{n} we must rule out the existence of high Euler characteristic surfaces in the graph complement. To that end, we define the graph distance, d𝒢d_{\mathcal{G}}, of graphs in S3S^{3}, an analogue of bridge distance of links. In the spirit of Hartshorn [17] and Bachman-Schleimer [7] we show that the complexity of an essential surface is bounded below by the graph bridge distance:

Theorem 1.2.

Let Γ\Gamma be a graph in a closed, orientable 3-manifold MM which is in bridge position with respect to a Heegaard surface BB, so that Mn(Γ)M\smallsetminus n(\Gamma) is irreducible and boundary irreducible. Let SS be a properly embedded, orientable, incompressible, boundary-incompressible, non-boundary parallel surface in Mn(Γ)M\smallsetminus n(\Gamma). Then d𝒢(B,Γ)d_{\mathcal{G}}(B,\Gamma) is bounded above by 2(2g(S)+|S|1)2(2g(S)+|\partial S|-1).

In Section 2 we lay out the definitions of the various complexes and distances we will use, and prove Theorem 1.2. In Section 3, we prove Theorem 1.1.

2. Definitions

Given a link S3\mathcal{L}\subset S^{3}, a bridge sphere for \mathcal{L} is a sphere, BB, embedded in S3S^{3}, intersecting the link \mathcal{L} transversely, and dividing S3S^{3} into two 33-balls, VV and WW, so that there exist disks DVD_{V} and DWD_{W} properly embedded in VV and WW, respectively, so that VDV\mathcal{L}\cap V\subset D_{V} and WDW\mathcal{L}\cap W\subset D_{W} are each a collection of arcs.

In [16], Goda introduced the notion of a bridge sphere for a spatial θ\theta-graph, and this was extended by Ozawa in [23]. A bridge sphere for a (spatial) graph Γ\Gamma is a sphere, BB, embedded in S3S^{3}, instersecting Γ\Gamma transversely in the interior of edges, and dividing S3S^{3} into two 33-balls, VV and WW, so that there exist disks DVD_{V} and DWD_{W} properly embedded in VV and WW, respectively, so that ΓVDV\Gamma\cap V\subset D_{V} and ΓWDW\Gamma\cap W\subset D_{W} are each a collection of trees and/or arcs.

If BB is a bridge sphere for a link \mathcal{L}, then a bridge disk is a disk properly embedded in one of the components of (S3n())B)¯\overline{(S^{3}\smallsetminus n(\mathcal{L}))\smallsetminus B)}, whose boundary consists of exactly two arcs, meeting at their endpoints, with one arc essential in Bn()B\smallsetminus n(\mathcal{L}), and the other essential in n()\partial n(\mathcal{L}). We refer to the arc in the boundary of the disk that is contained in BB as a bridge arc. Similarly, if BB is a bridge sphere for a graph Γ\Gamma, then a graph-bridge disk is a disk properly embedded in one of the components of (S3n(Γ))B)¯\overline{(S^{3}\smallsetminus n(\Gamma))\smallsetminus B)}, whose boundary consists of exactly two arcs, meeting at their endpoints, with one arc essential in Bn(Γ)B\smallsetminus n(\Gamma), and the other essential in n(Γ)\partial n(\Gamma). We refer to the arc in the boundary of the disk that is contained in BB as a graph-bridge arc.

Definition 2.1.

The curve complex for a surface BB with (possibly empty) boundary is the complex with vertices corresponding to the isotopy classes of essential simple closed curves in BB, so that a collection of vertices defines a simplex if representatives of the corresponding isotopy classes can be chosen to be pairwise disjoint. We will denote the curve complex for a surface BB by 𝒞(B)\mathcal{C}(B).

Definition 2.2.

The arc and curve complex for a surface BB^{\prime} with boundary is the complex with vertices corresponding to the (free) isotopy classes of essential simple closed curves and properly embedded arcs in BB^{\prime}. A collection of vertices defines a simplex if representatives of the corresponding isotopy classes can be chosen to be pairwise disjoint. We will denote the arc and curve complex for a surface BB^{\prime} by 𝒜𝒞(B)\mathcal{AC}(B^{\prime}).

If BB is a surface embedded in a manifold, and a 1-dimensional complex intersects BB transversely, we will refer to the surface obtained by removing a neighborhood of the 1-complex by BB^{\prime}. We will often refer to 𝒞(B)\mathcal{C}(B^{\prime}) simply by 𝒞(B)\mathcal{C}(B), and 𝒜𝒞(B)\mathcal{AC}(B^{\prime}) simply by 𝒜𝒞(B)\mathcal{AC}(B).

Definition 2.3.

Let BB be a surface with at least two distinct, essential curves. Given two collections XX and YY of vertices in the complex 𝒞(B)\mathcal{C}(B) (resp., 𝒜𝒞(B)\mathcal{AC}(B)), the distance between XX and YY , denoted d𝒞(B)(X,Y)d_{\mathcal{C}(B)}(X,Y) (resp., d𝒜𝒞(B)(X,Y)d_{\mathcal{AC}(B)}(X,Y)), is the minimal number of edges in any path in 𝒞(B)\mathcal{C}(B) (resp., 𝒜𝒞(B)\mathcal{AC}(B)) from a vertex in XX to a vertex in YY. When the surface is understood, we often just write d𝒞d_{\mathcal{C}} (resp., d𝒜𝒞d_{\mathcal{AC}}).

We will be working with four subtly different but closely related sub-complexes, and some associated notions of distance.

Definition 2.4.

Let BB be a properly embedded surface separating a manifold MM into two components, VV and WW. Define the disk set of VV (resp., WW), denoted 𝒟V𝒞(B)\mathcal{D}_{V}\subset\mathcal{C}(B), (resp. 𝒟W𝒞(B)\mathcal{D}_{W}\subset\mathcal{C}(B)), as the set of all vertices corresponding to essential simple closed curves in BB that bound embedded disks in VV (resp., WW). Define the disk set of BB, denoted 𝒟B\mathcal{D}_{B}, as the set of all vertices corresponding to essential simple closed curves in BB that bound embedded disks in MM.

Definition 2.5.

Let BB be a bridge sphere for a link \mathcal{L}, bounding 33-balls VV and WW, with at least 66 marked points corresponding to the transverse intersections of \mathcal{L} with BB. The distance of the bridge surface, denoted d𝒞(B,)d_{\mathcal{C}}(B,\mathcal{L}), is d𝒞(B)(𝒟V,𝒟W)d_{\mathcal{C}(B^{\prime})}(\mathcal{D}_{V},\mathcal{D}_{W}), the distance in the curve complex of BB^{\prime} between 𝒟V\mathcal{D}_{V} and 𝒟W\mathcal{D}_{W}.

The fundamental building block in our construction will be the exterior of a graph that is highly complex as viewed from the arc and curve complex. The existence of such a block will follow from a result of Blair, Tomova, and Yoshizawa. It is a special case of Corollary 5.3 from [9].

Theorem 2.6 ([9]).

Given non-negative integers bb and dd, with b3b\geq 3, there exists a 22-component link \mathcal{L} in S3S^{3}, and a bridge sphere BB for \mathcal{L} so that \mathcal{L} is bb-bridge with respect to BB and d𝒞(B,)dd_{\mathcal{C}}(B,\mathcal{L})\geq d.

Definition 2.7.

Let BB be a bridge sphere for a link \mathcal{L}, bounding 33-balls VV and WW. Define the bridge disk set of VV (resp., WW), denoted 𝒟V𝒜𝒞(B)\mathcal{BD}_{V}\subset\mathcal{AC}(B) (resp., 𝒟W\mathcal{BD}_{W}), as the set of all vertices either corresponding to essential simple closed curves in BB^{\prime} that bound embedded disks in VV\smallsetminus\mathcal{L} (resp., WW\smallsetminus\mathcal{L}), or corresponding to bridge arcs in BB^{\prime}.

Definition 2.8.

Let BB be a bridge sphere for a link \mathcal{L}, bounding 33-balls VV and WW. The bridge distance of the bridge surface BB, denoted d𝒟(B,)d_{\mathcal{BD}}(B,\mathcal{L}) is d𝒜𝒞(B)(𝒟V,𝒟W)d_{\mathcal{AC}(B^{\prime})}(\mathcal{BD}_{V},\mathcal{BD}_{W}), the distance in the arc and curve complex of BB^{\prime} between 𝒟V\mathcal{BD}_{V} and 𝒟W\mathcal{BD}_{W}.

Lemma 2.9 ([8], Lemma 2).

If BB is a bridge surface which is not a sphere with four or fewer punctures, then d𝒟(B,)d𝒞(B,)2d𝒟(B,)d_{\mathcal{BD}}(B,\mathcal{L})\leq d_{\mathcal{C}}(B,\mathcal{L})\leq 2d_{\mathcal{BD}}(B,\mathcal{L}).

Definition 2.10.

Let BB be a bridge sphere for graph Γ\Gamma, bounding 3-balls VV and WW. The graph disk set of VV (resp., WW) denoted 𝒢𝒟V𝒜𝒞(B)\mathcal{GD}_{V}\subset\mathcal{AC}(B) (resp., 𝒢𝒟W𝒜𝒞(B)\mathcal{GD}_{W}\subset\mathcal{AC}(B)), is the set of all vertices either corresponding to essential simple closed curves in Bn(Γ)B\smallsetminus n(\Gamma) that bound embedded disks in Vn(Γ)V\smallsetminus n(\Gamma) (resp., Wn(Γ)W\smallsetminus n(\Gamma)), or corresponding to graph-bridge arcs in Bn(Γ)B\smallsetminus n(\Gamma).

Definition 2.11.

Let BB be a bridge sphere for graph Γ\Gamma. The graph distance of the bridge surface, denoted d𝒢(B,Γ)d_{\mathcal{G}}(B,\Gamma) is d𝒜𝒞(B)(𝒢𝒟V,𝒢𝒟W)d_{\mathcal{AC}(B^{\prime})}(\mathcal{GD}_{V},\mathcal{GD}_{W}), the distance in the arc and curve complex of B=Bn(Γ)B^{\prime}=B\smallsetminus n(\Gamma) between 𝒢𝒟V\mathcal{GD}_{V} and 𝒢𝒟W\mathcal{GD}_{W}.

Lemma 2.12.

Let \mathcal{L} be a link in bridge position with respect to bridge sphere BB, bounding 3-balls VV and WW, and let Γ\Gamma_{\mathcal{L}} be a graph in bridge position with respect to BB formed by adding edges to \mathcal{L} in VV that are simultaneously parallel into BB in the complement of \mathcal{L}, and so that ΓV\Gamma_{\mathcal{L}}\cap V has at least two components.

If D(Vn(Γ))D\subset(V\smallsetminus n(\Gamma_{\mathcal{L}})) is a graph-bridge disk for Γ\Gamma_{\mathcal{L}}, then there is a bridge disk DD^{\prime} for \mathcal{L} in (Vn())(V\smallsetminus n(\mathcal{L})) which is disjoint from DD.

Proof.

Let Γ1\Gamma_{1}, …, Γ\Gamma_{\ell} be the connected components ΓV\Gamma_{\mathcal{L}}\cap V, and let Γi\Gamma_{i} be the component of ΓV\Gamma_{\mathcal{L}}\cap V to which DD is incident.

Over all bridge disks EVE\subset V for \mathcal{L} disjoint from Γi\Gamma_{i}, choose one which minimizes |DE||D\cap E|. Suppose the intersection is non-empty. Any loops of intersection can be removed because (Vn(Γ))(V\smallsetminus n(\Gamma)) is a handlebody and therefore irreducible. Any points of intersection between D\partial D and E\partial E are contained in DB\partial D\cap B and EB\partial E\cap B. Choose an arc γ\gamma of |DE||D\cap E|. The arc γ\gamma cuts DD into two disks Dγ1D_{\gamma_{1}} and Dγ2D_{\gamma_{2}}. For one of i=1i=1 or 22, DγiD\partial D_{\gamma_{i}}\cap\partial D is contained in BB. Call that disk DγD_{\gamma}. Consider an arc α\alpha of |DE||D\cap E| outermost in DγD_{\gamma}. If the interior of DγD_{\gamma} is disjoint from EE then take α\alpha to be γ\gamma. The arc α\alpha cuts off a disk DαD_{\alpha} from DγD_{\gamma} and cuts EE into two disks E1E_{1} and E2E_{2} only one of whose (say E2E_{2}) boundary is incident to \mathcal{L}. The disk E2Dα=EE_{2}\cup D_{\alpha}=E^{\prime} is a bridge disk for \mathcal{L} and intersects DD fewer times than EE, contradicting the minimality of |DE||D\cap E|. ∎

The above implies that the distance in the arc and curve complex of Bn(Γ)B\smallsetminus n(\Gamma) between 𝒢𝒟V\mathcal{GD}_{V} and 𝒟V\mathcal{BD}_{V} is less than or equal to one.

Corollary 2.13.

Let \mathcal{L} and Γ\Gamma_{\mathcal{L}} be as above. Then d𝒟(B,)1+d𝒢(B,Γ)d_{\mathcal{\mathcal{BD}}}(B,\mathcal{L})\leq 1+d_{\mathcal{G}}(B,\Gamma_{\mathcal{L}}).

Proof.

Since Wn(Γ)W\smallsetminus n(\Gamma) contains no graph-bridge disks, 𝒢𝒟W=𝒟W\mathcal{GD}_{W}=\mathcal{BD}_{W}. Thus d𝒢(B,Γ)=d𝒜𝒞(𝒢𝒟V,𝒟W)d_{\mathcal{G}}(B,\Gamma_{\mathcal{L}})=d_{\mathcal{AC}}(\mathcal{GD}_{V},\mathcal{BD}_{W}). Lemma 2.12 shows that d𝒜𝒞(𝒢𝒟V,𝒟V)1d_{\mathcal{AC}}(\mathcal{GD}_{V},\mathcal{BD}_{V})\leq 1, and so by the triangle inequality we have that d𝒟(B,)1+d𝒢(B,Γ)d_{\mathcal{BD}}(B,\mathcal{L})\leq 1+d_{\mathcal{G}}(B,\Gamma_{\mathcal{L}}). ∎

In [17], Hartshorn proved that an essential closed surface in a 3-manifold creates an upper bound on the possible distances of Heegaard splittings of that manifold in terms of the genus of the essential surface.

Theorem 2.14 (Hartshorn, Theorem 1.2 of [17]).

Let MM be a Haken 3-manifold containing an incompressible surface of genus gg. Then any Heegaard splitting of MM has distance at most 2g2g.

This idea has been generalized in numerous ways, including by Bachman and Schleimer, who show in [7] that the distance of a bridge Heegaard surface in a knot complement is bounded by twice the genus plus the number of boundary components of an essential properly embedded surface.

Theorem 2.15 (Bachman-Schleimer, Theorem 5.1 of [7]).

Let KK be a knot in a closed, orientable 3-manifold MM which is in bridge position with respect to a Heegaard surface BB. Let SS be a properly embedded, orientable, essential surface in Mn(K)M\smallsetminus n(K). Then the distance of KK with respect to BB is bounded above by twice the genus of SS plus |S||\partial S|.

We will need a yet more general version, since we will be concerned with surfaces properly embedded in graph complements.

The essence of both results is that the distance of a bridge or Heegaard surface is bounded above in terms of the complexity of an essential properly embedded surface. We will generalize this result to link and graph complements, with the additional benefit of avoiding many of the technical details of [7] necessary to treat the boundary components. Unfortunately, our bound will be worse than that obtained by Bachman and Schleimer, though it will be sufficient for many applications of this type of bound (e.g., [20], [15], [22], [5], and [21]). We note also that our proof requires a minimal starting position similar to that used by Hartshorn, an assumption the Bachman-Schleimer method was able to avoid.

We now prove the following. See 1.2

Proof of Theorem 1.2.

In the case that SS is closed, we note that the proofs of both Theorem 2.15 and Theorem 2.14 apply to closed surfaces in manifolds with boundary as long as the manifold is irreducible. In the case that S\partial S\neq\emptyset we will double Mn(Γ)M\smallsetminus n(\Gamma) along n(Γ)\partial n(\Gamma) to obtain a closed surface and show that the surface can be made to fulfill all the hypotheses necessary to use the machinery in the proof of Theorem 2.14 to obtain the bound on distance.

First, isotope SS to intersect BB minimally, among all isotopy representatives of SS. Let VV and WW be the handlebodies on either side of BB. Double Mn(Γ)M\smallsetminus n(\Gamma) along n(Γ)\partial n(\Gamma), and call the resulting manifold M^\widehat{M}. Let the doubles of SS, BB, VV and WW be S^\widehat{S}, B^\widehat{B}, V^\widehat{V} and W^\widehat{W}, respectively, and let GG be n(Γ)\partial n(\Gamma) in M^\widehat{M}, with respective copies MiM_{i}, SiS_{i}, BiB_{i}, ViV_{i} and WiW_{i} for i=1,2i=1,2.

Note that B^\widehat{B} is a Heegaard surface for M^\widehat{M}. (The proof of this is very similar to the proof of Proposition 3.2 below.) Also, note that since SS is incompressible and \partial-incompressible in Mn(Γ)M\smallsetminus n(\Gamma), S^\widehat{S} is an incompressible closed surface in M^\widehat{M} and since n(Γ)\partial n(\Gamma) was incompressible in Mn(Γ)M\smallsetminus n(\Gamma), GG is incompressible in M^\widehat{M}.

Claim 1.

Each of S^V^\widehat{S}\cap\widehat{V} and S^W^\widehat{S}\cap\widehat{W} are incompressible.

Proof.

If, say, S^V^\widehat{S}\cap\widehat{V} had a compressing disk DD, then since S^\widehat{S} is incompressible in M^\widehat{M}, there would have to be a disk DD^{\prime} in S^\widehat{S} with D=D\partial D^{\prime}=\partial D, and DB^D^{\prime}\cap\widehat{B}\neq\emptyset. We may choose DD to be a compressing disk which intersects GG minimally. Further, since GG is incompressible, we may choose DD to intersect GG only in arcs, if at all. But M^\widehat{M} is irreducible, so DDD\cup D^{\prime} bounds a ball and we may isotope S^\widehat{S} across this ball from DD^{\prime} to DD, lowering the number of intersections between S^\widehat{S} and B^\widehat{B}.

If DG=D^{\prime}\cap G=\emptyset, then this can be viewed as an isotopy of SS in Mn(Γ)M\smallsetminus n(\Gamma) which reduces the number of intersections between SS and BB, a contradiction.

If DGD^{\prime}\cap G\neq\emptyset we still arrive at a contradiction. Consider a loop, \ell, of intersection in (DD)G(D\cup D^{\prime})\cap G, innermost in DDD\cup D^{\prime}. Since DGD\cap G only contains arcs, \ell consists of two arcs, α\alpha and α\alpha^{\prime} in DD and DD^{\prime} respectively. Thus \ell bounds a disk DD_{\ell} in GG, α\alpha cuts off a subdisk DαD_{\alpha} of DD and α\alpha^{\prime} cuts off a subdisk DαD_{\alpha^{\prime}} of DD^{\prime}, both of which are in either M1M_{1} or M2M_{2}, say M1M_{1}. Now we have an isotopy of S1S_{1} from DαDαD_{\alpha}\cup D_{\alpha^{\prime}} to DD_{\ell}

Independent of whether DαD_{\alpha^{\prime}} intersected BB, we could have chosen DD to have fewer intersections with GG, contradicting our choice of DD to minimize intersections. ∎

Claim 2.

Every intersection of S^\widehat{S} with B^\widehat{B} is essential in B^\widehat{B}.

Proof.

Curves of intersection in S^B^\widehat{S}\cap\widehat{B} which are inessential in both surfaces would either give rise to a reduction in |SB||S\cap B| or could have come from the doubling of arcs in SBS\cap B which would give rise to a reduction in |SB||S\cap B| in a fashion similar to the previous claim. ∎

Claim 3.

There are no \partial-parallel annular components of S^W^\widehat{S}\cap\widehat{W} or S^V^\widehat{S}\cap\widehat{V}.

Proof.

Any such component disjoint from GG would have been eliminated when |SB||S\cap B| was minimized. The intersection of any such component intersecting GG with M1M_{1} would be a \partial-parallel disk which also would have been eliminated when |SB||S\cap B| was minimized. ∎

Now we have satisfied all the hypotheses to obtain the sequence of isotopic copies of S^\widehat{S} described in Lemmas 4.4 and 4.5 of [17]. Depending on whether either of S^V^\widehat{S}\cap\widehat{V} or S^W^\widehat{S}\cap\widehat{W} contain disk components or not, we apply either Lemma 4.4 or 4.5, respectively, of [17] to obtain a sequence of compressions of S^\widehat{S} which give rise to a path in 𝒜𝒞(S^)\mathcal{AC}(\widehat{S}). A priori, this path would not restrict to a path in 𝒜𝒞(S)\mathcal{AC}(S), but the following Claim shows that we can choose the compressions to be symmetric across GG, and so each compression will correspond to an edge in 𝒜𝒞(S)\mathcal{AC}(S).

Claim 4.

If there exists an elementary \partial-compression of S^\widehat{S} in V^\widehat{V} (resp. W^\widehat{W}), then there exists an elementary compression of S^\widehat{S} in V^\widehat{V} (resp. W^\widehat{W}) which is symmetric across GG in the sense that either

  1. (1)

    the \partial-compressing disk D1D_{1} is disjoint from GG in M1M_{1}, and there is a corresponding \partial-compressing disk D2D_{2} in M2M_{2}, or

  2. (2)

    the \partial-compression is along a disk that is symmetric across GG.

Proof.

Let DD be an elementary \partial-compression disk for, say, S^V^\widehat{S}\cap\widehat{V} chosen to minimize |DG||D\cap G|. We may restrict attention to such disks with |DG|>0|D\cap G|>0.

First, we observe that DGD\cap G cannot contain any loops of intersection, for a loop of DGD\cap G innermost in DD bounds a sub-disk of DD which would either give rise to a compression for GG or would provide a means of isotoping DD so as to lower |DG||D\cap G|. Thus, DGD\cap G consists only of arcs. These arcs are either

  • vertical arcs: with one endpoint on each of S^\widehat{S} and B^\widehat{B},

  • S^\widehat{S}-arcs: with both endpoints on S^\widehat{S}, or

  • B^\widehat{B}-arcs: with both endpoints on B^\widehat{B}.

Consider an S^\widehat{S}-arc of DGD\cap G, outermost in DD, cutting off sub-disk DD^{\prime} from DD, with boundary consisting of σ\sigma in S^\widehat{S} and γ\gamma in GG. Without loss of generality, assume DM1D^{\prime}\subset M_{1}. If σ\sigma is essential in S^M1\widehat{S}\cap M_{1}, then DD^{\prime} is a boundary compression disk for SS in MM, which is impossible. If σ\sigma is inessential in S^M1\widehat{S}\cap M_{1}, then it must co-bound a disk EE in S^M1\widehat{S}\cap M_{1} together with an arc σ(S^M1)\sigma^{\prime}\subseteq\partial(\widehat{S}\cap M_{1}). The curve γσ\gamma\cup\sigma^{\prime} cannot be essential in GG, else DED^{\prime}\cup E would be a compressing disk for GG. Thus, γσ\gamma\cup\sigma^{\prime} bounds a disk, FGF\subseteq G. Now FDEF\cup D^{\prime}\cup E is a sphere bounding a ball in M1M_{1}, so DED\cup E is isotopic to FF, and replacing DD^{\prime} with FF results in an elementary boundary compressing disk for S^V\widehat{S}\cap V with fewer intersections with GG than DD. Thus we may assume that DGD\cap G contains no S^\widehat{S}-arcs.

Now consider a sub-disk DD^{\prime} of DD which is cut off by all the arcs of DGD\cap G and whose boundary consists of no more than one vertical arc. With out loss of generality, assume DM1D^{\prime}\subseteq M_{1}. Suppose D\partial D^{\prime} has B^\widehat{B}-arcs, β1,β2,,βk\beta_{1},\beta_{2},\dots,\beta_{k}. Then all the βi\beta_{i} are disjoint arcs on GG. If any of them are inessential in GV^G\cap\widehat{V} then they bound disks BiGV1B_{i}\subseteq G\cap V_{1}. If any of the βi\beta_{i} are essential in GV^G\cap\widehat{V}, then they bound disks BiV1B_{i}\subseteq V_{1} that are bridges disks for n(Γ)n(\Gamma) in V1V_{1}. In either case, D(i=1kBi)D^{\prime}\cup\left(\bigcup_{i=1}^{k}B_{i}\right) results in a boundary compressing disk for SV^S\cap\widehat{V} with fewer intersections with GG than DD. This boundary compressing disk is still elementary as the arc in S^\widehat{S} remains unchanged. Thus, we may assume that DGD\cap G consists solely of vertical arcs.

Let γ\gamma be an arc of DGD\cap G outermost in DD, cutting off a sub-disk D1D_{1} from DD. Without loss of generality, D1M1D_{1}\subseteq M_{1}. The boundary of D1D_{1} consists of three arcs; γG\gamma\subseteq G, σ1S1\sigma_{1}\subseteq S_{1} and β1B1\beta_{1}\subseteq B_{1}. By symmetry, there exists disk D2M2D_{2}\subseteq M_{2} in M2M_{2}, so that D1D2D_{1}\cup D_{2} is a disk in V^\widehat{V} with boundary consisting of arcs σ=σ1σ2S^\sigma=\sigma_{1}\cup\sigma_{2}\subseteq\widehat{S} and β=β1β2B^\beta=\beta_{1}\cup\beta_{2}\subseteq\widehat{B}, intersecting GG in exactly one arc, γ\gamma. Finally, we must show that σ\sigma is a “strongly essential” arc in S^V^\widehat{S}\cap\widehat{V}.

If σ\sigma is not strongly essential then it is either the meridian of a boundary parallel annulus of S^V^\widehat{S}\cap\widehat{V} which is

not possible since σ1\sigma_{1} was a sub-arc of the original elementary compression disk DD, or σ\sigma is inessential in S^V^\widehat{S}\cap\widehat{V}. If σ\sigma is inessential then it would co-bound a disk EE in S^\widehat{S} together with an arc σS^B^\sigma^{\prime}\subseteq\widehat{S}\cap\widehat{B}. This disk provides an isotopy in S^\widehat{S} of σ1\sigma_{1} to σ2\sigma_{2}.

If the disk D=DD1D^{\prime}=D\smallsetminus D_{1} only intersects D2D_{2} in γ\gamma then DD2D^{\prime}\cup D_{2} is a compressing disk for S^V^\widehat{S}\cap\widehat{V} with fewer arcs of intersection with GG, as the disk can be isotoped away from γ\gamma. This disk is still an elementary compressing disk because σ1\sigma_{1} is isotopic to σ2\sigma_{2}, and so contradicts our original choice of DD.

Thus, σ\sigma is strongly essential in S^V^\widehat{S}\cap\widehat{V}, and D1D2D_{1}\cup D_{2} is a new compressing disk for S^V^\widehat{S}\cap\widehat{V} that is symmetric across GG. ∎

We may, thus, proceed exactly as in Theorem 2.14. Each elementary boundary compression of S^\widehat{S} towards either of V^\widehat{V} or W^\widehat{W} can be performed in a symmetric way, demonstrating a path from 𝒟V^\mathcal{D}_{\widehat{V}} to 𝒟W^\mathcal{D}_{\widehat{W}} in 𝒞(S^)\mathcal{C}(\widehat{S}) of length no greater than twice the genus of S^\widehat{S}, which is 2(g(S)+|S|1)2(g(S)+|\partial S|-1).

Each time a boundary compression for S^\widehat{S} corresponds to a pair of curves ci^\widehat{c_{i}} and ci+1^\widehat{c_{i+1}} in S1S_{1} that contribute an edge in a path in 𝒞(S^)\mathcal{C}(\widehat{S}) from 𝒟V^\mathcal{D}_{\widehat{V}} to 𝒟W^\mathcal{D}_{\widehat{W}}, there is immediately a pair of curves ci+2^\widehat{c_{i+2}} and ci+3^\widehat{c_{i+3}} in S2S_{2} also contributing an edge in a path from 𝒟V\mathcal{D}_{V} to 𝒟W\mathcal{D}_{W}, and this pair of paths corresponds to a single pair of curves cic_{i} and ci+1c_{i+1} in SS contributing a single edge in 𝒜𝒞(S)\mathcal{AC}(S). Each time a boundary compression for S^\widehat{S} corresponds to a pair of curves intersecting GG that contributes an edge in a path in 𝒞(S^)\mathcal{C}(\widehat{S}) from 𝒟V^\mathcal{D}_{\widehat{V}} to 𝒟W^\mathcal{D}_{\widehat{W}}, the restriction of these curves to S1S_{1} is a pair of arcs contributing an edge in 𝒜𝒞(S)\mathcal{AC}(S).

Further, since the boundary compressions (and elimination of boundary parallel annuli) are all being performed symmetrically, the resulting disks DV^𝒟V^D_{\widehat{V}}\in\mathcal{D}_{\widehat{V}} from S^V^\widehat{S}\cap\widehat{V} and DW^𝒟W^D_{\widehat{W}}\in\mathcal{D}_{\widehat{W}} from S^W^\widehat{S}\cap\widehat{W} are symmetric. That is, either DV^D_{\widehat{V}} (resp., DW^D_{\widehat{W}}) is disjoint from GG, so that we may assume that it sits in V1V_{1} (resp., W1W_{1}), or it is symmetric across GG so that DV^M1D_{\widehat{V}}\cap M_{1} (resp., DW^M1)D_{\widehat{W}}\cap M_{1}) is a graph bridge disk for Γ\Gamma in MM. In either case, this demonstrates a path in 𝒜𝒞(S)\mathcal{AC}(S) from 𝒟𝒢V\mathcal{DG}_{V} to 𝒟𝒢W\mathcal{DG}_{W} of length no greater than 2(g(S)+|S|1)2(g(S)+|\partial S|-1). ∎

3. Theorem 1.1

In [4] Bachman defined the topological index of a surface. In contrast to the distances between sub-complexes each corresponding to some disks discussed in Section 2, he exploits the homotopy type of the complex of all disks.

Definition 3.1.

The surface BB is said to be topologically minimal if either 𝒟B\mathcal{D}_{B} is empty, or if there exists an nn\in\mathbb{N} so that πn(𝒟B)0\pi_{n}(\mathcal{D}_{B})\neq 0. If a surface BB is topologically minimal, then the topological index is defined to be the smallest nn\in\mathbb{N} so that πn1(𝒟B)0\pi_{n-1}(\mathcal{D}_{B})\neq 0, or 0 if 𝒟B\mathcal{D}_{B} is empty.

In [6] Johnson and Bachman showed that surfaces of arbitrarily high index exist, but the manifolds they construct all contain essential tori. We prove an analogue of this.

See 1.1

3.1. The construction

Let nn be a positive integer. We will construct a hyperbolic manifold containing a Heegaard surface of topological index nn.

Using the machinery in Theorem 2.6, let \mathcal{L} be a (0,4)(0,4)-link in S3S^{3} with two components, LL and KK, with bridge sphere BB of distance at least 32n+732n+7. Let VV and WW be the two 3-balls bounded by BB. Since \mathcal{L} is in bridge position, there exist disks DVD_{V} and DWD_{W} properly embedded in VV and WW, respectively, with (V)DV(\mathcal{L}\cap V)\subset D_{V}, and (W)DW(\mathcal{L}\cap W)\subset D_{W}. By modifying DVD_{V} if necessary, we can find two arcs τL\tau_{L} and τK\tau_{K} in BB such that

  1. (1)

    τLτKDV\tau_{L}\cup\tau_{K}\subset D_{V},

  2. (2)

    τLτK=\tau_{L}\cap\tau_{K}=\emptyset,

  3. (3)

    τL=τLL\tau_{L}\cap\mathcal{L}=\partial\tau_{L}\subset L and τK=τKK\tau_{K}\cap\mathcal{L}=\partial\tau_{K}\subset K,

  4. (4)

    each of τK\tau_{K} and τL\tau_{L} have endpoints on different components of V\mathcal{L}\cap V.

Let L=LτLL^{\prime}=L\cup\tau_{L}, let GL=n(L)G_{L}=\partial n(L^{\prime}), let K=KτKK^{\prime}=K\cup\tau_{K}, let GK=n(K)G_{K}=\partial n(K^{\prime}), and let Γ=τLτK=LK\Gamma=\mathcal{L}\cup\tau_{L}\cup\tau_{K}=L^{\prime}\cup K^{\prime}. Observe that Γ\Gamma is a graph in bridge position with respect to BB. Let M=S3n(Γ)¯M^{\prime}=\overline{S^{3}\smallsetminus n(\Gamma)}, let V=Vn(Γ)¯V^{\prime}=\overline{V\smallsetminus n(\Gamma)}, and let W=Wn(Γ)¯=Wn()¯W^{\prime}=\overline{W\smallsetminus n(\Gamma)}=\overline{W\smallsetminus n(\mathcal{L})}, and B=Bn(Γ)=Bn()B^{\prime}=B\smallsetminus n(\Gamma)=B\smallsetminus n(\mathcal{L}).

For each i=1,2,,ni=1,2,\dots,n, let MiM^{\prime}_{i} be homeomorphic to MM^{\prime}, along with homeomorphic copies i\mathcal{L}_{i} of \mathcal{L}, (GL)i(G_{L})_{i} of GLG_{L}, (GK)i(G_{K})_{i} of GKG_{K}, and BiB^{\prime}_{i} of BB^{\prime}.

Then, for each i=1,2,,(n1)i=1,2,\dots,(n-1), identify (GK)i(G_{K})_{i} with (GL)i+1(G_{L})_{i+1} and identify (GK)n(G_{K})_{n} with (GL)1(G_{L})_{1}, all via the same homeomorphism. Call the resulting closed 33-manifold MnM^{n}. Observe that the union of the BiB^{\prime}_{i} is a closed surface that we will call BnB^{n}. We will show that BnB^{n} is a Heegaard surface for MnM^{n}, that BnB^{n} has high topological index, and that MnM^{n} is hyperbolic.

Proposition 3.2.

For each nn, the surface BnMnB^{n}\subset M^{n} is a genus 3n+13n+1 Heegaard surface.

Proof.

That the genus of BnB^{n} is 3n+13n+1 can be verified by an Euler characteristic count. It suffices, then, to verify that the complement of BnB^{n} is two handlebodies, VnV^{n} and WnW^{n}.

Since Γ\Gamma was in bridge position with respect to BB, there are disks DVD_{V} and DWD_{W} properly embedded in VV and WW, respectively, so that ΓVDV\Gamma\cap V\subset D_{V} and ΓWDW\Gamma\cap W\subset D_{W}. Then DVD_{V} and DWD_{W} cut along Γ\Gamma is a collection of sub-disks.

The result of cutting Vn(Γ)V\smallsetminus n(\Gamma) along all these sub-disks of DVD_{V} is a pair of 3-balls, each with two sub-disks, D1+D_{1}^{+} and D2+D_{2}^{+}, of n(Γ)n(\Gamma) contained in the boundary. Each identification of (GK)i(G_{K})_{i} with (GL)i+1(G_{L})_{i+1} (indices mod nn) glues pairs of these sub-disks along arcs, resulting in disks in VnV^{n}, and further cutting along (n1)(n-1) copies of each of D1+D_{1}^{+} and D2+D_{2}^{+} results in a collection of 33-balls, showing that VnV^{n} is a handlebody.

Similarly, the result of cutting Wn(Γ)W\smallsetminus n(\Gamma) along all of the sub-disks of DWD_{W} is a pair of 3-balls, each with four sub-disks of n(Γ)n(\Gamma) contained in the boundary, D1,D2,D3D_{1}^{-},D_{2}^{-},D_{3}^{-}, and D4D_{4}^{-}. Each identification of (GK)i(G_{K})_{i} with (GL)i+1(G_{L})_{i+1} (indices mod nn) glues pairs of these sub-disks along arcs, resulting in disks in WnW^{n}, and further cutting along (n1)(n-1) copies of each of D1,D2,D3D_{1}^{-},D_{2}^{-},D_{3}^{-}, and D4D_{4}^{-} results in a collection of 33-balls, showing that WnW^{n} is a handlebody. ∎

3.2. Bounding from above

Proposition 3.3.

The surface SnS^{n} has topological index at most nn.

Proof.

Our proof will follow almost exactly as the proof of Proposition 5 from [6]. In each copy MiM_{i}^{\prime} of the manifold MM^{\prime}, we have the surface BiB^{\prime}_{i}, a copy of BB^{\prime}, dividing the manifold into ViV_{i}^{\prime} and WiW_{i}^{\prime}, copies of VV^{\prime} and WW^{\prime}. Observe that in each ViV^{\prime}_{i}, there is exactly one essential disk, Di+D_{i}^{+} with boundary contained in BiB_{i}^{\prime}, just as in [6]. However, in each WiW_{i}^{\prime}, there are several essential disks with boundary contained in BiB_{i}^{\prime}. We will call this collection of disks 𝒟i\mathscr{D}^{-}_{i}. From each 𝒟i\mathscr{D}^{-}_{i}, choose a single representative DiD^{-}_{i}.

Define the sub-complex, PP, of 𝒟M\mathcal{D}_{M} spanned by the vertices corresponding to i{Di+,Di}\bigcup_{i}\{D_{i}^{+},D_{i}^{-}\}, which is homeomorphic to an (n1)(n-1)-sphere. Then, define a map F:𝒟MPF:\mathcal{D}_{M}\to P by the identity on PP, and by sending a vertex corresponding to a disk Di{Di+,Di}D\not\in\bigcup_{i}\{D_{i}^{+},D_{i}^{-}\} to the vertex corresponding to Dj+D_{j}^{+} or DjD_{j}^{-}, where either D𝒟jD\in\mathscr{D}_{j}^{-}, or jj is the smallest index for which an essential outermost sub-disk of D(iGi)D\smallsetminus(\bigcup_{i}G_{i}) is contained in VjV^{\prime}_{j} or WjW^{\prime}_{j}, respectively.

Just as in [6], we claim that this map FF is a simplicial map that fixes each vertex of PP. To see this, consider any two disks D1D_{1} and D2D_{2} connected by an edge in 𝒟M\mathcal{D}_{M} (so that the disks are realized disjointly in MM). Observe that by our construction of MM^{\prime} and Corollary 2.13, any disk contained in VjV^{\prime}_{j} must intersect any disk contained in WjW^{\prime}_{j} (whether either disk is a bridge disk, a graph-bridge disk, or the boundary is contained in BjB^{\prime}_{j}). So, if Di±=F(D1)F(D2)=Dj±D_{i}^{\pm}=F(D_{1})\neq F(D_{2})=D_{j}^{\pm}, then iji\neq j, and F(D1)F(D_{1}) is joined to F(D2)F(D_{2}) in PP. Thus, FF is a retraction onto the (n1)(n-1)-sphere, PP, showing that πn1(𝒟M)\pi_{n-1}(\mathcal{D}_{M}) is non-trivial, so the topological index of BnB^{n} is at most nn. ∎

Corollary 3.4.

The topological index of BnB^{n} is well-defined, and BnB^{n} is topologically minimal.

3.3. Bounding from below

We make use of an important theorem in the development of topological index by Bachman:

Theorem 3.5 (Theorem 3.7 of [4]).

Let GG be a properly embedded, incompressible surface in an irreducible 3-manifold MM. Let BB be a properly embedded surface in MM with topological index nn. Then BB may be isotoped so that

  1. (1)

    BB meets GG in pp saddles, for some pnp\leq n, and

  2. (2)

    the sum of the topological indices of the components of Bn(G)B\smallsetminus n(G), plus pp is at most nn.

Proposition 3.6.

The surface BnB^{n} has topological index no smaller than nn.

Proof.

Suppose SnS^{n} had topological index ι<n\iota<n. By Theorem 3.5, BnB^{n} can be isotoped to a surface, B0nB^{n}_{0}, so that B0nB^{n}_{0} meets H=n(G)H=n(G) in σ\sigma saddles, the sum of the topological indices of each component of B0nn(H)B^{n}_{0}\smallsetminus n(H) is kk, and k+σιk+\sigma\leq\iota. Further, we may isotope any annular components of B0nHB^{n}_{0}\smallsetminus H that are boundary parallel into H\partial H completely into HH. Observe that this will have no effect on the Euler characteristic of B0nHB^{n}_{0}\smallsetminus H, nor any effect on the topological index, since such a component will have topological index zero. We consider two different cases.

First, suppose that there is some component of B0nHB^{n}_{0}\smallsetminus H with Euler characteristic less than 8n-8n. In this case, because the Euler characteristic of B0nB^{n}_{0} is 6n-6n, the sum of the Euler characteristics of the remaining components of B0nHB^{n}_{0}\smallsetminus H must be greater than 2n2n. This implies that there are at least n+1n+1 components of B0nHB^{n}_{0}\smallsetminus H with non-negative Euler characteristic. Again, as the sum of the topological indices of each component of B0nHB^{n}_{0}\smallsetminus H is k<nk<n, there must be at least one component of B0nHB^{n}_{0}\smallsetminus H with non-negative Euler characteristic and topological index zero. This is impossible by Theorem 1.2.

Second, suppose that the Euler characteristic of each component of B0nHB^{n}_{0}\smallsetminus H is bounded below by 8n-8n. As the sum of the topological indices of each component of B0nHB^{n}_{0}\smallsetminus H is k<nk<n, there must be at least one index jj so that every component of B0nMjB^{n}_{0}\cap M_{j} has topological index zero. Thus, there is a component, B′′B^{\prime\prime}, of B0nMjB^{n}_{0}\cap M_{j} which is incompressible and has Euler characteristic bounded below by 8n-8n.

While B′′B^{\prime\prime} may be boundary compressible, we may boundary compress B′′B^{\prime\prime} maximally, if necessary, to obtain a surface that is incompressible, boundary incompressible, and not boundary parallel. Since boundary compressions only increase Euler characteristic, the resulting essential surface has Euler characteristic bounded below by 8n-8n.

By Lemma 2.9 and Corollary 2.13, in MjM_{j} with BjB_{j} a copy of BB^{\prime}, we have d𝒞(Bj,)2d𝒟(Bj,)2(1+d𝒢(Bj,Γ))d_{\mathcal{C}}(B_{j},\mathcal{L})\leq 2d_{\mathcal{BD}}(B_{j},\mathcal{L})\leq 2(1+d_{\mathcal{G}}(B_{j},\Gamma)). By Theorem 1.2, d𝒢(Bj,Γ)2(2g(B′′)+|B′′|1)d_{\mathcal{G}}(B_{j},\Gamma)\leq 2(2g(B^{\prime\prime})+|\partial B^{\prime\prime}|-1). By our choice of \mathcal{L} and the fact that χ(S)=22g(S)|S|\chi(S)=2-2g(S)-|\partial S|, we have 32n+7d𝒞(Bj,)2+2d𝒢(Bj,Γ)8g(B′′)+4|B′′|2=4χ(B′′)+632n+7\leq d_{\mathcal{C}}(B_{j},\mathcal{L})\leq 2+2d_{\mathcal{G}}(B_{j},\Gamma)\leq 8g(B^{\prime\prime})+4|\partial B^{\prime\prime}|-2=-4\chi(B^{\prime\prime})+6. On the other hand we have just shown that 8nχ(B′′)-8n\leq\chi(B^{\prime\prime}), a contradiction. In either case, we find that the topological index of BnB^{n} cannot be less than nn. ∎

3.4. Hyperbolicity

We have now shown that MnM^{n} contains a surface of topological index nn. To prove Theorem 1.1 it remains to show that MnM^{n} is hyperbolic.

Proposition 3.7.

For n>1n>1, MnM^{n} is hyperbolic.

Proof.

Consider an essential surface SS in MnM^{n} with Euler characteristic bounded below by zero, chosen to intersect GG minimally. If SG=S\cup G=\emptyset, we arrive at a contradiction to Theorem 1.2 as SS would lie in one of the copies of MM^{\prime}. If SGS\cup G\neq\emptyset, the incompressibility and boundary incompressibility of GG guarantees that the curves of SGS\cup G are essential in SS. Thus SMiS\cap M^{\prime}_{i} is a collection of one or more planar surfaces for some ii. This again contradicts Theorem 1.2. Thus, in particular, MnM^{n} is prime and atoridal for all nn. Then, as GG is an incompressible surface in MnM^{n}, we conclude that MnM^{n} is hyperbolic. ∎

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