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Rigidity results for large displacement quotients of mapping class groups

Giorgio Mangioni (Giorgio Mangioni) Maxwell Institute and Department of Mathematics, Heriot-Watt University, Edinburgh, UK gm2070@hw.ac.uk
Abstract.

We consider quotients of mapping class groups of orientable, finite type surfaces by subgroups whose action on the curve graph has large displacement. This class includes quotients by the normal closure of a pseudo-Anosov element, the mapping class group itself, and in view of forthcoming work of Abbott-Berlyne-Ng-Rasmussen also random quotients. First, we show that every automorphism of the corresponding quotient of the curve graph is induced by a mapping class, thus generalising Ivanov’s Theorem about automorphisms of the curve graph. Then we use this to prove quasi-isometric rigidity under additional assumptions, satisfied by all aforementioned quotients. In the process, we clarify a proof of quasi-isometric rigidity of mapping class groups by Behrstock, Hagen, and Sisto. Finally, we show that the outer automorphisms groups of our quotients, as well as their abstract commensurators, are “the smallest possible”.

Introduction

In recent years there has been a growing interest in studying quotients and subgroups of mapping class groups of orientable, finite type surfaces, in order to establish the analogues of Ivanov’s theorem about automorphisms of the curve graph and its consequences (see e.g. [BM19, McL19] for a wide class of normal subgroups, and, among others, [MS23] for quotients by large enough powers of Dehn Twists).

In this paper, we address the problem for a class of quotients which we call large displacement quotients. The defining property, articulated in Definition 1.2, is that every non-trivial element in the kernel acts with large displacement on the curve graph of the surface, that is, the distance between any vertex and its image is bounded from below by a large enough constant, which we call the minimum displacement. An example of such behaviour is the quotient by the normal closure of some power of a pseudo-Anosov element, which was studied in e.g. [DGO17] to answer questions about the existence of normal free subgroups of 𝒞𝒢±(S)\mathcal{MCG}^{\pm}(S). Furthermore, the definition applies to the mapping class group itself, seen as the quotient by the trivial subgroup.

We have three main results, which we think of as rigidity properties of our quotients. The first one is a generalisation of a celebrated theorem of Ivanov-Korkmaz [Iva97, Kor99], and morally tells us that all properties of a large displacement quotient are already encoded in the action on the corresponding quotient of the curve graph. Here 𝒞𝒢±(S)\mathcal{MCG}^{\pm}(S) denotes the extended mapping class group, where we allow orientation-reversing mapping classes.

Theorem 1.

Let SS be a surface of complexity at least 33 which is not S2,0S_{2,0}, and let N𝒞𝒢±(S)N\unlhd\mathcal{MCG}^{\pm}(S) be a normal subgroup. If the minimum displacement of NN is large enough, then the map 𝒞𝒢±(S)/NAut(𝒞S/N)\mathcal{MCG}^{\pm}(S)/N\to\text{Aut}(\mathcal{C}S/N), induced by the action of 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N on 𝒞S/N\mathcal{C}S/N, is an isomorphism.

The bound on the minimum displacement is made precise in Theorem 2.1. A similar result holds for some surfaces of low complexity too, but in these cases the map might only be surjective with finite kernel (see Subsection 2.1 for the details).

In the second half of the paper, we restrict our attention to those large displacement quotients admitting a hierarchically hyperbolic group (HHG) structure, in the sense of [BHS19]. We also require the structure to be “inherited” from the standard HHG structure of the mapping class group, in a sense that is clarified in Convention 3.2. Roughly, we ask that the domain set of the HHG structure consists almost exclusively of all NN-orbits of surfaces, that the top-level coordinate space coincides with 𝒞S/N\mathcal{C}S/N, and that the coordinate space of the orbit of a subsurface USU\subsetneq S is quasi-isometric to the curve graph of UU. The class of quotients admitting such a HHG structure, which we call “surface-inherited”, includes:

  • the mapping class group itself (by e.g. [BHS19, Theorem 11.1]);

  • the quotient by the normal closure of a power of a pseudo-Anosov element (by [BHS17a, Corollary F]);

  • more generally, quotients by “deep enough” subgroups of hierarchically hyperbolically embedded subgroups, in the sense of [BHS17a, Definition 6.1] (see Lemma 3.5 for details);

  • in view of forthcoming work of Abbott-Berlyne-Ng-Rasmussen, also random quotients of 𝒞𝒢±(S)\mathcal{MCG}^{\pm}(S).

For such quotients, we can state our second main result, which is quasi-isometric rigidity. Recall that two groups GG and HH are weakly commensurable if there exist two finite normal subgroups LHL\unlhd H and MGM\unlhd G such that the quotients H/LH/L and G/MG/M have two finite index subgroups that are isomorphic.

Theorem 2.

Let SS be a surface of complexity at least 22 which is not a torus with two punctures, and let N𝒞𝒢±(S)N\unlhd\mathcal{MCG}^{\pm}(S) be a normal subgroup. If the minimum displacement of NN is large enough, and if 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N has a surface-inherited HHG structure, then 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N is quasi-isometrically rigid, meaning that if a finitely generated group GG and 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N are quasi-isometric then they are weakly commensurable.

Since 𝒞𝒢±(S)\mathcal{MCG}^{\pm}(S) itself is a large displacement quotient, we also recover quasi-isometric rigidity of mapping class groups, first proven in [BKMM12].

Finally, combining quasi-isometric rigidity and results on automorphisms of acylindrically hyperbolic groups from [AMS16], we are able to deduce the following, which can be regarded as a form of algebraic rigidity and is a generalisation of a result of Ivanov for mapping class groups [Iva97]:

Theorem 3 (Algebraic rigidity).

Let SS be either a surface of complexity at least 33 (excluding the case S=S2,0S=S_{2,0}) or a S0,5S_{0,5}, and let 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N be a large displacement quotient with a surface-inherited HHG structure. If the minimum displacement is large enough, then the following facts hold:

  1. (1)

    The map 𝒞𝒢±(S)/NAut(𝒞𝒢±(S)/N)\mathcal{MCG}^{\pm}(S)/N\to\text{Aut}(\mathcal{MCG}^{\pm}(S)/N), which maps every element to the corresponding inner automorphism, is an isomorphism. In particular, Out(𝒞𝒢±(S)/N)\text{Out}(\mathcal{MCG}^{\pm}(S)/N) is trivial.

  2. (2)

    The abstract commensurator of 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N coincides with 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N itself. In particular, any isomorphism between finite index subgroups of 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N is the restriction of an inner automorphism.

Sketch of proofs

Combinatorial rigidity

To show that any automorphism ϕ¯:𝒞S/N𝒞S/N\overline{\phi}:\,\mathcal{C}S/N\to\mathcal{C}S/N is induced by some element g¯𝒞𝒢±(S)/N\overline{g}\in\mathcal{MCG}^{\pm}(S)/N we proceed as follows. First, we find an automorphism ϕ:𝒞S𝒞S\phi:\mathcal{C}S\to\mathcal{C}S which “lifts” ϕ¯\overline{\phi}, i.e. that makes the following diagram commute, where π:𝒞S𝒞S/N\pi:\,\mathcal{C}S\to\mathcal{C}S/N is the quotient map:

𝒞S{\mathcal{C}S}𝒞S{\mathcal{C}S}𝒞S/N{\mathcal{C}S/N}𝒞S/N{\mathcal{C}S/N}ϕ\scriptstyle{\phi}π\scriptstyle{\pi}π\scriptstyle{\pi}ϕ¯\scriptstyle{\overline{\phi}}

The key observation is that, if we regard both 𝒞S\mathcal{C}S and 𝒞S/N\mathcal{C}S/N as simplicial complexes, then π\pi is a covering map (see Lemma 2.2). Moreover, by a result of Harer [Har86], 𝒞S\mathcal{C}S is simply connected whenever SS has large enough complexity, and we can lift ϕ¯\overline{\phi} by standard arguments of covering theory. Then one can apply a result of Ivanov-Korkmaz [Iva97, Kor99] to show that the lift ϕ\phi is induced by a mapping class g𝒞𝒢±(S)g\in\mathcal{MCG}^{\pm}(S), and therefore its image g¯𝒞𝒢±(S)/N\overline{g}\in\mathcal{MCG}^{\pm}(S)/N induces ϕ¯\overline{\phi}.

Quasi-isometric rigidity

We follow a general strategy, developed by Jason Behrstock, Mark Hagen, and Alessandro Sisto in [BHS21], to prove quasi-isometric rigidity of certain HHG. The key idea from that paper is that any self-quasi-isometry ff of a HHG, satisfying some additional assumptions, induces an automorphism of a certain graph, which should be thought of as encoding the intersection patterns of maximal quasiflats (that is, quasi-isometric embeddings of n\mathbb{R}^{n} of maximum dimension). In the case of 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N, such graph is precisely the quotient of the curve graph, since maximal quasiflats of 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N morally correspond to subgroups generated by maximal families of commuting Dehn Twists. But then, by the combinatorial rigidity results from Section 2, the automorphism of 𝒞S/N\mathcal{C}S/N is induced by some element g¯𝒞𝒢±(S)/N\overline{g}\in\mathcal{MCG}^{\pm}(S)/N, and with a little more effort one can show that ff coarsely coincides with the left multiplication by g¯\overline{g}.

In [BHS21], the main result to extract combinatorial data from a self-quasi-isometry of a HHG is [BHS21, Theorem 5.7], which is then used in [BHS21, Theorem 5.10] to give a new proof of quasi-isometric rigidity of mapping class groups. Unfortunately, as pointed out by Jason Behrstock after that paper was published, [BHS21, Theorem 5.7] does not apply to mapping class groups. Indeed, if UU is a subsurface of complexity 11, then any maximal collection of pairwise disjoint subsurfaces that contains UU must also contain the boundary annuli of UU. Hence, mapping class groups do not satisfy [BHS21, Assumption 2], which roughly states that such a UU should be the only subsurface shared by two maximal collections of pairwise disjoint subsurfaces.

Behrstock, Hagen, and Sisto, worked out a modification of their Assumptions which allows them to prove a version of [BHS21, Theorem 5.7] which applies to the mapping class group. Rather than writing their argument separately, they instead opted to allow me to incorporate a version of those assumptions into this work, and I am extremely grateful for this possibility. Then the proof of [BHS21, Theorem 5.10] runs verbatim once one replaces [BHS21, Theorem 5.7] with our Lemma 3.18, whose Assumptions (A) - (F) are satisfied by both 𝒞𝒢±(S)\mathcal{MCG}^{\pm}(S) and our quotients (see Lemma 3.20).

We stress that [BHS21, Theorem 5.7] is true as stated, and it is also used in [DDLS21] to study quasi-isometric rigidity of extensions of Veech groups.

Algebraic rigidity

Given an isomorphism ϕ:HH\phi:\,H\to H^{\prime} between finite-index subgroups of 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N, one can consider the element g¯𝒞𝒢±(S)/N\overline{g}\in\mathcal{MCG}^{\pm}(S)/N whose left-multiplication coarsely coincides with ϕ\phi, seen as a self-quasi-isometry of 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N, and then try to prove that the conjugation by g¯\overline{g} restricts to the given isomorphism on HH. We do just that in Theorem 4.1, using tools from [AMS16] for acylindrical group actions on hyperbolic spaces. We can use such tools since, by [BHS17b, Corollary 14.4], 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N acts acylindrically on the top-level coordinate space of the HHG structure, which coincides with 𝒞S/N\mathcal{C}S/N for those quotients satisfying Convention 3.2. Notice that finite normal subgroups could cause the outer automorphism group to be finite rather than trivial, so the key technical results we need is that 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N does not contain non-trivial finite normal subgroups, Lemma 4.7.

Comparison with quotients by large powers of Dehn twists

Very similar results hold for quotients of the form 𝒞𝒢±(S)/DTK\mathcal{MCG}^{\pm}(S)/DT_{K}, where DTKDT_{K} is the normal subgroup generated by all KK-th powers of Dehn Twists. Such quotients can be regarded as “Dehn filling quotients” of mapping class groups, as pointed out and explored in [DHS21] and then in [BHMS20], where they are proven to be hierarchically hyperbolic. Moreover, in view of [MS23], they enjoy the same combinatorial, quasi-isometric, and algebraic rigidity properties as our quotients (at least when SS is a punctured sphere, and conjecturally also in the general case). While the proofs there also rely on lifting, the quotient map 𝒞S𝒞S/DTK\mathcal{C}S\to\mathcal{C}S/DT_{K} is not a covering map, and indeed it is quite far from being locally injective; therefore lifting properties follow from different technologies, involving results from [Dah18] about rotating families and the existence of finite rigid sets as defined in [AL13]. Moreover, in this paper quasi-isometric rigidity relies on the fact that Dehn twist flats survive in the quotient, while they disappear in the quotient by DTKDT_{K} for any choice of KK. In particular, quasi-isometries of 𝒞𝒢±(S)/DTK\mathcal{MCG}^{\pm}(S)/DT_{K} induce automorphisms of a graph which is not 𝒞S/DTK\mathcal{C}S/DT_{K}, and then one has to relate these two graphs with further combinatorial considerations.

Questions

The following question was asked by Jason Behrstock, during an exchange on a first draft of this paper:

Question 1.

Let SS be either a surface of complexity at least 33 (excluding the case S=S2,0S=S_{2,0}) or a S0,5S_{0,5}, and let 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N be a large displacement quotient with a surface-inherited HHG structure. Does there exist D0D\geq 0 such that, if the minimum displacement is at least DD, any injection from a finite index subgroup H𝒞𝒢±(S)/NH\leq\mathcal{MCG}^{\pm}(S)/N to 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N is induced by an inner automorphism?

This would be a strengthening of our Theorem 3, where we also require the image of the injection to have finite index. Indeed, our proof needs this further assumption, since we want to apply Theorem 2 in order to find a candidate element of 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N, and an isomorphism between subgroups is a quasi-isometry of 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N if and only if both its domain and image are of finite index.

Question 1 would also be a generalisation of the analogue results for mapping class groups, proved by Irmak in [Irm06a, Irm04, Irm06b] and then extended by Behrstock-Margalit in [BM06]. The main strategy of all these papers is articulated in two steps:

  • First, one proves that any superinjective map of 𝒞S\mathcal{C}S (that is, any self-map preserving adjacency and non-adjacency between vertices) is induced by an element of 𝒞𝒢±(S)\mathcal{MCG}^{\pm}(S). This is a generalisation of Ivanov’s combinatorial rigidity theorem, since a simplicial isomorphism is clearly superinjective.

  • Then one shows that any injection from a finite-index subgroup of 𝒞𝒢±(S)\mathcal{MCG}^{\pm}(S) into 𝒞𝒢±(S)\mathcal{MCG}^{\pm}(S) maps powers of Dehn Twists to powers of Dehn Twists, preserving commutation and non-commutation. Therefore the injection induces a superinjective map of 𝒞S\mathcal{C}S, and one finds a candidate element of 𝒞𝒢±(S)\mathcal{MCG}^{\pm}(S) whose conjugation restricts to the given injection.

Therefore, if we want to repeat the same argument for our quotients, we need to answer the following:

Question 2.

In the setting of Question 1, is any superinjective map of 𝒞S/N\mathcal{C}S/N induced by an element of 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N?

This would be a generalisation of Theorem 1, which I believe to be true. One could try to lift a superinjective map of 𝒞S/N\mathcal{C}S/N to a superinjective map of 𝒞S\mathcal{C}S, and then conclude by the results of Irmak and Behrstock-Margalit.

Question 3.

In the setting of Question 1, does the injection H𝒞𝒢±(S)/NH\to\mathcal{MCG}^{\pm}(S)/N map powers of Dehn Twists to powers of Dehn Twist?

Irmak proof is ultimately a refined version of Ivanov’s characterisation of Dehn Twists from [Iva88], in terms of the centres of their centralisers in 𝒞𝒢±(S)\mathcal{MCG}^{\pm}(S), which might extend to our quotients. I believe this is one more reason to try to understand better centralisers in hierarchically hyperbolic groups.

Outline of the paper

In Section 1 we gather some examples of the quotients 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N by subgroups with large displacement, and we develop the lifting tools that are used throughout the paper.

In Section 2 we prove combinatorial rigidity for the general case, which is Theorem 2.1, and for some low-complexity surfaces, see Subsection 2.1. This establishes Theorem 1.

Section 3 is devoted to the proof of Theorem 2. First, we show that a self-quasi-isometry of a hierarchically hyperbolic space, satisfying certain properties (which are Assumption (A) - (F)), induce an automorphism of a certain graph, which encodes the intersections of certain maximal quasiflats (see Lemma 3.18). Then in Subsection 3.5 we relate such graph to 𝒞S/N\mathcal{C}S/N, and in the proof of Theorem 3.8 we use the combinatorial rigidity results from Section 2 to produce an element of 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N whose left-multiplication is within finite distance from the quasi-isometry.

We conclude the paper with Section 4, where we use quasi-isometric rigidity and some tools from [AMS16] about acylindrical actions on hyperbolic spaces to show that any automorphism between finite index subgroups of 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N is the restriction of the conjugation by a unique element g¯𝒞𝒢±(S)/N\overline{g}\in\mathcal{MCG}^{\pm}(S)/N (see Theorem 4.1 for the existence of such an element, and Lemma 4.8 for the uniqueness). Therefore, the outer automorphism group of 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N, as well as its abstract commensurator, are the smallest possible, as clarified in Corollaries 4.9 and 4.10. This proves the two parts of Theorem 3.

Acknowledgements

I would like to thank Jason Behrstock, Mark Hagen, and Alessandro Sisto for sharing with me their previous attempts to find a different set of assumptions under which the conclusion of [BHS21, Theorem 5.7] holds, and for suggesting many corrections to the first draft of this paper. I am especially grateful to my supervisor Alessandro Sisto for his constant support. I am also grateful to Piotr Przytycki for suggesting a way to shorten the proof of Theorem 2.8. Finally, I thank Carolyn Abbott, Daniel Berlyne, Thomas Ng, and Alexander Rasmussen for fruitful discussions.

1. Large displacement quotients

Let SS be a surface of finite type, that is, a surface obtained from a closed, connected, oriented surface after removing a finite number of points, called punctures. When we want to emphasise the genus gg and the number of punctures bb we will use the notation Sg,bS_{g,b}, and we will denote by ζ(S)=3g+b3\zeta(S)=3g+b-3 the complexity of Sg,bS_{g,b}. Let 𝒞S\mathcal{C}S be the curve graph of SS, whose vertices are (isotopy classes of) curves and adjacency corresponds to disjointness. Whenever it will not cause ambiguity, we will always say “curve” to mean its isotopy class. Finally, let 𝒞𝒢±(S)\mathcal{MCG}^{\pm}(S) be the extended mapping class group of SS, where we allow orientation-reversing mapping classes. If x𝒞S(0)x\in\mathcal{C}S^{(0)} is a curve and f𝒞𝒢±(S)f\in\mathcal{MCG}^{\pm}(S) is a mapping class, we will denote the image of xx under ff simply by fxfx.

Let us introduce which quotients of 𝒞𝒢±(S)\mathcal{MCG}^{\pm}(S) we are considering.

Definition 1.1 (Minimum displacement).

The minimum displacement of a mapping class f𝒞𝒢±(S)f\in\mathcal{MCG}^{\pm}(S) is defined as minx𝒞S(0)d𝒞S(x,fx)\min_{x\in\mathcal{C}S^{(0)}}\mathrm{d}_{\mathcal{C}S}(x,fx). Similarly, the minimum displacement of a subgroup N𝒞𝒢±(S)N\leq\mathcal{MCG}^{\pm}(S) is defined as

minfN{1}minx𝒞S(0)d𝒞S(x,fx),\min_{f\in N-\{1\}}\min_{x\in\mathcal{C}S^{(0)}}\mathrm{d}_{\mathcal{C}S}(x,fx),

where 1𝒞𝒢±(S)1\in\mathcal{MCG}^{\pm}(S) is the identity.

Definition 1.2 (Large displacement quotient).

Let N𝒞𝒢±(S)N\unlhd\mathcal{MCG}^{\pm}(S) be a normal subgroup, and let D>0D\in\mathbb{N}_{>0}. We will say that the quotient group 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N is a DD-large displacement quotient if the minimum displacement of NN is at least DD.

Here are some examples of this behaviour.

Example 1.3.

Definition 1.2 applies to the trivial subgroup N={1}N=\{1\}, thus 𝒞𝒢±(S)\mathcal{MCG}^{\pm}(S) itself is a DD-large displacement quotient for every D>0D\in\mathbb{N}_{>0}.

Example 1.4.

Let f𝒞𝒢±(S)f\in\mathcal{MCG}^{\pm}(S) be a pseudo-Anosov element. For every D>0D\in\mathbb{N}_{>0} one can find some large enough K>0K\in\mathbb{N}_{>0} such that fKf^{K} has minimum displacement at least DD. Moreover, up to choosing a larger KK, the quotient by the normal closure N=fKN=\langle\langle f^{K}\rangle\rangle is a DD-large displacement quotient. We will give a proof in Corollary 3.6, after we have developed some more notation.

1.1. Isometric projections

Let 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N be a DD-large displacement quotient. Since NN acts on 𝒞S\mathcal{C}S by simplicial automorphisms, we can consider the quotient 𝒞S/N\mathcal{C}S/N by this action. Here we gather some properties of 𝒞S/N\mathcal{C}S/N and the projection map π:𝒞S𝒞S/N\pi:\,\mathcal{C}S\to\mathcal{C}S/N, which hold whenever DD is large enough:

Lemma 1.5.

Let 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N be a DD-large displacement quotient. If D3D\geq 3 then 𝒞S/N\mathcal{C}S/N is a simplicial graph.

Proof.

By definition of quotient by a simplicial action, there is an edge in 𝒞S/N\mathcal{C}S/N between two vertices x¯,y¯𝒞S/N(0)\overline{x},\overline{y}\in\mathcal{C}S/N^{(0)} if they admit two adjacent representatives in 𝒞S\mathcal{C}S. First notice that, by the assumption on the minimum displacement, two vertices in the same NN-orbit cannot be adjacent, hence no edge of 𝒞S/N\mathcal{C}S/N connects a vertex to itself. Moreover, we claim that no two vertices x¯,y¯\overline{x},\overline{y} are connected by more than one edge. Indeed, if there were two edges between them, we could find two edges {x,y}\{x,y\} and {x,y}\{x^{\prime},y^{\prime}\} between representatives of x¯\overline{x} and y¯\overline{y}, respectively. We can further assume that y=yy=y^{\prime}, up to replacing {x,y}\{x^{\prime},y^{\prime}\} with one of its NN-translates. But then xx and xx^{\prime} would be NN-translate within distance at most 22, contradicting the fact that the minimum displacement is at least 33. ∎

Definition 1.6.

Let X¯\overline{X} be a subgraph of 𝒞S/N\mathcal{C}S/N. We say that a subgraph XX of 𝒞S\mathcal{C}S is a lift of X¯\overline{X} if the projection map π:𝒞S𝒞S/N\pi:\,\mathcal{C}S\to\mathcal{C}S/N restricts to an isometry between XX and X¯\overline{X}.

Lemma 1.7 (Isometric lifts and projections).

Let 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N be a DD-large displacement quotient. If D8D\geq 8 then the following facts hold for the projection π:𝒞S𝒞S/N\pi:\,\mathcal{C}S\to\mathcal{C}S/N:

  • π\pi is 11-Lipschitz;

  • For every combinatorial path Γ¯𝒞S/N\overline{\Gamma}\subset\mathcal{C}S/N there exists a combinatorial path Γ𝒞S\Gamma\subset\mathcal{C}S such that π(Γ)=Γ¯\pi(\Gamma)=\overline{\Gamma}, and moreover if Γ¯\overline{\Gamma} is geodesic then so is Γ\Gamma;

  • For every x𝒞S(0)x\in\mathcal{C}S^{(0)}, π\pi restricts to an isometry between the closed ball of radius 22 centred at xx, which we denote by B(x,2)B(x,2), and the closed ball of radius 22 centred at its projection x¯\overline{x}, which we denote by B¯(x¯,2)\overline{B}(\overline{x},2);

  • Every subgraph X¯\overline{X} of 𝒞S/N\mathcal{C}S/N which is contained in a closed ball of radius 22 admits a unique NN-orbit of lifts.

It is possible that our bound on DD can be sharpened. However this is irrelevant, since in all notable applications one is always allowed to replace NN with a suitable finite-index subgroup, in order to make the minimum displacement larger.

Proof.

The quotient map is 11-Lipschitz since the action of NN on 𝒞S\mathcal{C}S is simplicial. In order to find a combinatorial path Γ𝒞S\Gamma\subset\mathcal{C}S which projects to a given path Γ¯𝒞S/N\overline{\Gamma}\subset\mathcal{C}S/N it suffices to lift one edge at a time, given a lift of its starting point, and again this can be done since the action is simplicial. Notice that, by construction, Γ\Gamma has the same length of Γ¯\overline{\Gamma}. Moreover, suppose that Γ¯\overline{\Gamma} is a geodesic between its endpoints x¯,y¯\overline{x},\overline{y}, which lift to the endpoints x,yx,y of Γ\Gamma. Then, denoting by (Γ)\ell(\Gamma) the length of Γ\Gamma, and similarly for Γ¯\overline{\Gamma}, we get

d𝒞S(x,y)(Γ)=(Γ¯)=d𝒞S/N(x¯,y¯)d𝒞S(x,y),\mathrm{d}_{\mathcal{C}S}(x,y)\leq\ell(\Gamma)=\ell(\overline{\Gamma})=\mathrm{d}_{\mathcal{C}S/N}(\overline{x},\overline{y})\leq\mathrm{d}_{\mathcal{C}S}(x,y),

where we used that Γ¯\overline{\Gamma} realises the distance between x¯\overline{x} and y¯\overline{y}, and that the projection map is 11-Lipschitz. But then the inequalities above are all equalities, and in particular Γ\Gamma realises the distance between its endpoints, i.e., it is a geodesic path.

Now, let x𝒞S(0)x\in\mathcal{C}S^{(0)} and let x¯\overline{x} be its projection. Combining the previous points we have that π(B(x,2))=B¯(x¯,2)\pi(B(x,2))=\overline{B}(\overline{x},2), so we are left to show that, for every y,zB(x,2)y,z\in B(x,2), we have that d𝒞S/N(y¯,z¯)=d𝒞S(y,z)\mathrm{d}_{\mathcal{C}S/N}(\overline{y},\overline{z})=\mathrm{d}_{\mathcal{C}S}(y,z), where y¯\overline{y} and z¯\overline{z} are the respective projections. If by contradiction this was not the case, then we could pick any geodesic Γ¯\overline{\Gamma} between y¯\overline{y} and z¯\overline{z}. Notice that, since y,zB(x,2)y,z\in B(x,2) and π\pi is 11-Lipschitz, we have that d𝒞S/N(y¯,z¯)4\mathrm{d}_{\mathcal{C}S/N}(\overline{y},\overline{z})\leq 4, thus Γ¯\overline{\Gamma} must have length at most 33. Now lift Γ¯\overline{\Gamma} to a geodesic path Γ\Gamma starting at yy and ending at some zz^{\prime} in the same orbit of zz. But then zz and zz^{\prime} would be within distance at most 77, contradicting the assumption on the minimum displacement.

For the last statement, every subgraph X¯\overline{X} which is contained in a closed 22-ball admits a lift, by applying the local inverse of π\pi. Given any two lifts X,XX,X^{\prime}, let xXx\in X and xXx^{\prime}\in X^{\prime} be two points with the same projection, so that there exists an element nNn\in N such that x=nxx^{\prime}=nx. Now pick another pair yXy\in X and yXy^{\prime}\in X^{\prime} with the same projection. Since yy^{\prime} and nyny are within distance at most 44, by the assumption on the minimum displacement we must have that y=nyy^{\prime}=ny. Hence nX=XnX=X^{\prime}, that is, all lifts belong to the same NN-orbit. ∎

1.2. Orbits of subsurfaces

We conclude the Section with a study of how NN acts on the subsurfaces of SS. We first recall a definition from [BKMM12, Section 2.1.3]:

Definition 1.8.

A subsurface USU\subset S is essential if it is the disjoint union of some components of the complement of a collection of disjoint simple closed curves, so that no component is a pair of pants and no two annuli components are isotopic.

Let 𝔖\mathfrak{S} be the collection of (isotopy classes of) essential subsurfaces. Whenever it will not cause ambiguity, we will always say “subsurface” to mean its isotopy class. Moreover, if U𝔖U\in\mathfrak{S} is an annulus, then it is the regular neighbourhood of some curve x𝒞S(0)x\in\mathcal{C}S^{(0)}, which we call the core of UU.

Two subsurfaces U,V𝔖U,V\in\mathfrak{S} are nested (resp. orthogonal), and we write UVU\sqsubseteq V (resp. UVU\bot V) if UU is contained in VV (resp. if they are disjoint). If U,VU,V are neither \sqsubseteq-related nor orthogonal, then they are transverse and we write UVU\pitchfork V.

Now let 𝔖¯=𝔖/N\overline{\mathfrak{S}}=\mathfrak{S}/N be the collection of NN-orbits of subsurfaces. We will denote the equivalence class of a subsurface U𝔖U\in\mathfrak{S} by U¯\overline{U}, and similarly if 𝒰={Ui}iI\mathcal{U}=\{U_{i}\}_{i\in I} is a collection of subsurfaces we will set 𝒰¯={U¯i}iI\overline{\mathcal{U}}=\{\overline{U}_{i}\}_{i\in I}. Two classes U¯,V¯𝔖¯\overline{U},\overline{V}\in\overline{\mathfrak{S}} are nested (resp. orthogonal), and we write U¯V¯\overline{U}\sqsubseteq\overline{V} (resp. U¯V¯\overline{U}\bot\overline{V}) if there exists at least one pair of representatives U,VU,V such that UVU\sqsubseteq V (resp. UVU\bot V). Notice that we are not requiring that all pairs of representatives are nested (resp. orthogonal), and indeed this is almost never the case. If U¯,V¯\overline{U},\overline{V} are neither \sqsubseteq-related nor orthogonal, then they are transverse and we write U¯V¯\overline{U}\pitchfork\overline{V}.

Lemma 1.9.

Let 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N be a DD-large displacement quotient. If D2D\geq 2 then nesting and orthogonality in 𝔖¯\overline{\mathfrak{S}} are mutually exclusive, meaning that if U¯V¯𝔖¯\overline{U}\sqsubseteq\overline{V}\in\overline{\mathfrak{S}} then U¯⊥̸V¯\overline{U}\not\bot\overline{V}.

Proof.

Let U,VU,V be two representatives such that UVU\sqsubseteq V, and let xx be a curve which lies in UU. By the assumption on the minimum displacement, for every nN{1}n\in N-\{1\} the curve nxnx, which lies in nUnU, must intersect xx. This means that any representative for U¯\overline{U} cannot be disjoint from xx, and therefore from VV.

Now let UU¯U^{\prime}\in\overline{U} and VV¯V^{\prime}\in\overline{V} be any two representatives, and let nNn^{\prime}\in N such that nV=Vn^{\prime}V=V^{\prime}. Then the pair (U,V)(U^{\prime},V^{\prime}) is the image under nn^{\prime} of ((n)1U,V)((n^{\prime})^{-1}U,V), and by the previous argument we know that the latter two subsurfaces intersect. Hence UU^{\prime} intersects VV^{\prime}, that is, any representative for V¯\overline{V} is not disjoint from any representative for U¯\overline{U}. ∎

Lemma 1.10.

Let 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N be a DD-large displacement quotient for some D4D\geq 4 and let U¯1,,U¯k𝔖¯\overline{U}_{1},\ldots,\overline{U}_{k}\in\overline{\mathfrak{S}} be a collection of pairwise orthogonal elements. Then there exist representatives U1,,Uk𝔖U_{1},\ldots,U_{k}\in\mathfrak{S} which are pairwise orthogonal.

Notice that this lemma is not at all obvious: we just know that every two elements of the collection admit disjoint representatives, but this does not mean, a priori, that this conditions can all be satisfied simultaneously.

Proof.

The proof is by induction on kk, the base case k=2k=2 being true by how we defined orthogonality. Thus let k>2k>2 and let U1,U2U_{1},U_{2} be disjoint representatives for U¯1,U¯2\overline{U}_{1},\overline{U}_{2}. Moreover, let U3U¯3U_{3}\in\overline{U}_{3} be such that U3U1U_{3}\bot U_{1} (such representative exists since we know that U¯1,U¯3\overline{U}_{1},\overline{U}_{3} admit disjoint representatives, and up to the NN-action we can assume that the representative for U¯1\overline{U}_{1} is U1U_{1}). Similarly, there exists nNn\in N such that nU3U2nU_{3}\bot U_{2}.

Now fix a curve xU1x\in U_{1}. First notice that every curve yy lying on U3U_{3} is disjoint from xx. Moreover, nyny is disjoint from all curves on U2U_{2}, which are in turn disjoint from xx. Hence d𝒞S(y,ny)3\mathrm{d}_{\mathcal{C}S}(y,ny)\leq 3, and by the assumption on the minimum displacement we must have that n=1n=1. Thus U3U_{3} is disjoint from both U1U_{1} and U2U_{2}. If we repeat the procedure we can find representatives UiU¯iU_{i}\in\overline{U}_{i} for every i=3,,ki=3,\ldots,k which are disjoint from both U1U_{1} and U2U_{2}. Hence we can replace U1U_{1} and U2U_{2} with the subsurface U1U2U_{1}\sqcup U_{2}, and now the conclusion follows by induction. ∎

2. Combinatorial rigidity

For the rest of the paper, 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N will be a DD-large displacement quotient for some constant D8D\geq 8, so that all results from Subsections 1.1 and 1.2 hold. The 𝒞𝒢±(S)\mathcal{MCG}^{\pm}(S)-action on 𝒞S\mathcal{C}S induces an action of 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N on 𝒞S/N\mathcal{C}S/N, defined as follows: for every equivalence classes g¯𝒞𝒢±(S)/N\overline{g}\in\mathcal{MCG}^{\pm}(S)/N and x¯𝒞S/N\overline{x}\in\mathcal{C}S/N we can choose representatives gg and xx and set g¯x¯=gx¯\overline{g}\cdot\overline{x}=\overline{gx}. Using that NN is a normal subgroup, one can see that the definition is well-posed. Moreover, the action is by simplicial automorphism, since it preserves adjacency. Thus we have a group homomorphism 𝒞𝒢±(S)/NAut(𝒞S/N)\mathcal{MCG}^{\pm}(S)/N\to\text{Aut}(\mathcal{C}S/N), where Aut(𝒞S/N)\text{Aut}(\mathcal{C}S/N) is the group of simplicial automorphisms of 𝒞S/N\mathcal{C}S/N.

The goal of this Section is to prove the following, which is Theorem 1 from the Introduction. For the sake of simplicity, we will first state the result for surfaces of complexity at least 33 which are not S2,0S_{2,0}, postponing low-complexity cases to Subsection 2.1.

Theorem 2.1 (Combinatorial rigidity).

Let SS be a surface of complexity at least 33 which is not S2,0S_{2,0}, and let 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N be a DD-large displacement quotient. If D8D\geq 8 then the map 𝒞𝒢±(S)/NAut(𝒞S/N)\mathcal{MCG}^{\pm}(S)/N\to\text{Aut}(\mathcal{C}S/N), induced by the natural action, is an isomorphism.

For this Section only, it is convenient to see 𝒞S\mathcal{C}S and 𝒞S/N\mathcal{C}S/N as simplicial complexes, that is, we consider the flag simplicial complexes whose 11-skeleton are the curve graph and its quotient, respectively. By a result of Harer [Har86], if SS has complexity at least 33 then 𝒞S\mathcal{C}S is simply connected. We can show that 𝒞S\mathcal{C}S is actually the universal cover of 𝒞S/N\mathcal{C}S/N:

Lemma 2.2.

Let 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N be a DD-large displacement quotient. If D8D\geq 8 then the projection π:𝒞S𝒞S/N\pi:\,\mathcal{C}S\to\mathcal{C}S/N is a covering map.

Proof.

Just notice that, for every point p𝒞Sp\in\mathcal{C}S, there exists an open neighbourhood UU whose preimage is the disjoint union of open subsets which are homeomorphic to UU via π\pi. Indeed, for every p𝒞Sp\in\mathcal{C}S, choose a clique Δ\Delta that contains pp, and let xx be any of its vertices. Then we can choose UU to be the interior of the subcomplex spanned by B(x,2)B(x,2), as a consequence of Lemma 1.7. ∎

Proof of Theorem 2.1.

We first argue that the map 𝒞𝒢±(S)/NAut(𝒞S/N)\mathcal{MCG}^{\pm}(S)/N\to\text{Aut}(\mathcal{C}S/N) is surjective, i.e. that, given an automorphism ϕ¯Aut(𝒞S/N)\overline{\phi}\in\text{Aut}(\mathcal{C}S/N), we can find an element g¯𝒞𝒢±(S)/N\overline{g}\in\mathcal{MCG}^{\pm}(S)/N which induces ϕ¯\overline{\phi}. Since π:𝒞S𝒞S/N\pi:\,\mathcal{C}S\to\mathcal{C}S/N is the universal cover, there exists a continuous map ϕ:𝒞S𝒞S\phi:\,\mathcal{C}S\to\mathcal{C}S that makes the following diagram commute:

𝒞S{\mathcal{C}S}𝒞S{\mathcal{C}S}𝒞S/N{\mathcal{C}S/N}𝒞S/N{\mathcal{C}S/N}ϕ\scriptstyle{\phi}π\scriptstyle{\pi}π\scriptstyle{\pi}ϕ¯\scriptstyle{\overline{\phi}}

Recall that ϕ\phi is defined as follows: fix a vertex x0𝒞Sx_{0}\in\mathcal{C}S and a lift x1x_{1} of ϕ¯(π(x0))\overline{\phi}(\pi(x_{0})). Then for every x𝒞Sx\in\mathcal{C}S pick any path Γ\Gamma from x0x_{0} to xx, and set ϕ(x)\phi(x) as the endpoint of the lift of ϕ¯(π(Γ))\overline{\phi}(\pi(\Gamma)) starting at x0x_{0}. In particular, if two vertices x,y𝒞S(0)x,y\in\mathcal{C}S^{(0)} are adjacent, then their images ϕ(x),ϕ(y)\phi(x),\phi(y) will either be adjacent or coincide. Moreover, the second happens precisely when π(x)=π(y)\pi(x)=\pi(y), and by the assumption on the minimum displacement this cannot happen for adjacent vertices.

Hence, at the level of the 11-skeleton, ϕ\phi is a simplicial map, and it is actually an automorphism since we can repeat the same argument replacing ϕ¯\overline{\phi} with its inverse ϕ¯1\overline{\phi}^{-1}. Hence, by Ivanov’s Theorem [Iva97, Kor99] there is an element g𝒞𝒢±(S)g\in\mathcal{MCG}^{\pm}(S) which induces ϕ\phi, and therefore its image g¯𝒞𝒢±(S)/N\overline{g}\in\mathcal{MCG}^{\pm}(S)/N induces ϕ¯\overline{\phi}.

Now we turn to injectivity. If an element g𝒞𝒢±(S)g\in\mathcal{MCG}^{\pm}(S) induces the identity on 𝒞S/N\mathcal{C}S/N when passing to the quotient, then the gg-action on 𝒞S\mathcal{C}S is a covering automorphism. Now, the group of covering automorphisms is the group NN itself, since by Definition 1.2 the NN-action on 𝒞S\mathcal{C}S is properly discontinuous. Thus there exists an element nNn\in N such that the composition gngn fixes every curve of 𝒞S\mathcal{C}S, and since SS has complexity at least 33 and is not an S2,0S_{2,0} we have that gngn must be the identity (see e.g. the discussion in [FM12, Section 3.4]). ∎

2.1. Some low-complexity cases

In this Subsection we establish an analogue of Theorem 2.1 for some surfaces of low complexity. Let us first consider the cases when SS is either S0,4S_{0,4}, S1,0S_{1,0} or S1,1S_{1,1}. Then the curve graph has a slightly different definition: we connect two (isotopy classes of) curves if and only if they realise the minimal intersection number among all pairs of curves on the surface, which is 11 for S1,0S_{1,0} and S1,1S_{1,1} and 22 for S0,4S_{0,4}. The resulting simplicial complex is the Farey complex (see e.g. [Min96] for a proof), which is a triangulation of the compactification of the hyperbolic plane and therefore is simply connected. Moreover, the definition of a DD-large displacement quotient and the relative Lemmas from Section 1 did not assume any property on the nature of the vertices of 𝒞S\mathcal{C}S, thus they still hold in our context. Then one gets the following:

Theorem 2.3.

Let SS be either S0,4S_{0,4}, S1,0S_{1,0} or S1,1S_{1,1}, let D8D\geq 8 and let 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N be a DD-large displacement quotient. Then the map 𝒞𝒢±(S)/NAut(𝒞S/N)\mathcal{MCG}^{\pm}(S)/N\to\text{Aut}(\mathcal{C}S/N) is surjective and has finite kernel K¯\overline{K}, generated by the images of the hyperelliptic involutions in Figure 1.

Proof.

For the surjectivity part, we can run the exact same proof of Theorem 2.1, which only uses that the covering space 𝒞S\mathcal{C}S is simply connected. Moreover, the injectivity part of that proof implies that, if g¯𝒞𝒢±(S)/N\overline{g}\in\mathcal{MCG}^{\pm}(S)/N acts trivially on 𝒞S/N\mathcal{C}S/N, then it is the image of an element g𝒞𝒢±(S)g\in\mathcal{MCG}^{\pm}(S) which acts trivially on 𝒞S\mathcal{C}S. Such gg must then lie in the finite subgroup generated by the hyperelliptic involutions in Figure 1 (again, this follows from e.g. [FM12, Section 3.4]). ∎

With the exact same procedure, one can get the following:

Theorem 2.4.

Let S=S2,0S=S_{2,0}, and let 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N be a DD-large displacement quotient. If D8D\geq 8 then the map 𝒞𝒢±(S)/NAut(𝒞S/N)\mathcal{MCG}^{\pm}(S)/N\to\text{Aut}(\mathcal{C}S/N) is surjective, and the kernel is the /2\mathbb{Z}/2\mathbb{Z} subgroup generated by the image of the hyperelliptic involution in Figure 1.

Refer to caption
Refer to caption
Figure 1. The dots represent the punctures. Rotations by π\pi about the indicated axes fix all curves on the surfaces.

Finally, leaving aside the case S=S1,2S=S_{1,2}, which is more involved since the natural map 𝒞𝒢(S1,2)Aut(𝒞S1,2)\mathcal{MCG}(S_{1,2})\to\text{Aut}(\mathcal{C}S_{1,2}) is not surjective (see the main result of [Luo00]), we are left to deal with the case S=S0,5S=S_{0,5}. The curve complex 𝒞S\mathcal{C}S has dimension 11 and is not simply connected. However, we shall see that we can repeat the same procedure as in Theorem 2.1 if we show that the polyhedral complex, obtained from 𝒞(S0,5)\mathcal{C}(S_{0,5}) by gluing a cell to every 55-cycle, is simply connected. The latter is an unpublished result of Piotr Przytycki, which I thank for explaining its proof to me.

First, by an arc we mean the isotopy class, relative to the punctures, of a map γ:[0,1]S0,5\gamma:\,[0,1]\to S_{0,5} mapping each endpoint of the interval to a puncture. For every surface SS with at least 22 punctures, let 𝒜2(S)\mathcal{A}^{2}(S) be the simplicial complex whose vertices are all arcs γ:[0,1]S0,5\gamma:\,[0,1]\to S_{0,5} whose endpoints are distinct punctures, and where a collection of arcs span a simplex if their interiors are pairwise disjoint.

Lemma 2.5.

If SS has at least two punctures, 𝒜2(S)\mathcal{A}^{2}(S) is simply-connected.

The same proof will yield that 𝒜2(S)\mathcal{A}^{2}(S) is contractible, though we will not need it.

Proof.

This fact is proven as [Sch20, Claim 3.17], but we spell out the details for clarity. Let γ:𝕊1𝒜2(S)\gamma:\,\mathbb{S}^{1}\to\mathcal{A}^{2}(S) be a simplicial loop, and fix an arc x0γx_{0}\in\gamma. If every other arc yγy\in\gamma is disjoint from x0x_{0}, then we can connect x0x_{0} to yy, and this defines an extension of γ\gamma to some triangulation of the disk D2D^{2}.

Thus, suppose that Σ(γ)=yγi(x,y)>0\Sigma(\gamma)=\sum_{y\in\gamma}i(x,y)>0, where i(x,y)i(x,y) is the number of intersection of two representatives of xx and yy in minimal position. Fix and endpoint p0p_{0} of x0x_{0}, and let y0γy_{0}\in\gamma be the first arc one meets when travelling along x0x_{0} starting from p0p_{0}. Let tt be the path along x0x_{0} from p0p_{0} to the first intersection to y0y_{0}, and let zz and zz^{\prime} be the essential arcs obtained as the boundaries of a regular neighbourhood of ty0t\cup y_{0}. Since y0y_{0} has distinct endpoints, one of its endpoints is not p0p_{0}, and therefore one of the new arcs, say zz, has distinct endpoints. Notice moreover that zz is disjoint from y0y_{0}, and if y1γy_{1}\in\gamma was disjoint from y0y_{0} then it is also disjoint from zz, because we choose y0y_{0} to have the closest intersection to p0p_{0}. Thus, we can replace y0y_{0} with zz and obtain a loop γ\gamma^{\prime}, which is homotopic to γ\gamma but is such that Σ(γ)<Σ(γ)\Sigma(\gamma^{\prime})<\Sigma(\gamma). Then we conclude by induction on Σ(γ)\Sigma(\gamma). ∎

Definition 2.6.

Let S=S0,5S=S_{0,5}. By a pentagon we mean a 55-cycle P𝒞SP\subset\mathcal{C}S. Let 𝒞SP\mathcal{C}S_{P} be the polyhedral complex obtained from 𝒞S\mathcal{C}S by gluing a 22-cell to every pentagon.

Lemma 2.7 (Przytycki).

The complex 𝒞SP\mathcal{C}S_{P} is simply connected.

Proof.

First, notice that 𝒞S\mathcal{C}S can be seen as a non-complete subgraph of 𝒜2(S)\mathcal{A}^{2}(S), by mapping every curve yy to the unique arc a(y)a(y) in the twice-punctured disk that yy cuts out on SS. The map a:𝒞S𝒜2(S)a:\,\mathcal{C}S\to\mathcal{A}^{2}(S) is bijective at the level of vertices, but not at the level of edges since in 𝒜2(S)\mathcal{A}^{2}(S) we allow two arcs to have the same endpoints. Notice moreover that, if the union of five arcs is a pentagon on SS (meaning that there is a cyclic ordering such that each arc intersects only the previous and the following, and only at a single endpoint), then the preimages under aa of these arcs form a pentagon, in the sense of Definition 2.6.

Now let γ:𝕊1𝒞SP\gamma:\,\mathbb{S}^{1}\to\mathcal{C}S_{P} be a simplicial loop, whose image lies in the 11-skeleton 𝒞SP(1)=𝒞S\mathcal{C}S_{P}^{(1)}=\mathcal{C}S. The image a(γ)𝒜2(S)a(\gamma)\subset\mathcal{A}^{2}(S) can be filled with triangles, since 𝒜2(S)\mathcal{A}^{2}(S) is simply connected. Let x0,x1,x2𝒜2(S)x_{0},x_{1},x_{2}\in\mathcal{A}^{2}(S) be the vertices of such a triangle TT. If xix_{i} and xjx_{j} have disjoint endpoints, then the corresponding curves a1(xi)a^{-1}(x_{i}) and a1(xj)a^{-1}(x_{j}) are disjoint, so that they are connected by an edge in 𝒞S\mathcal{C}S. Otherwise, there exists a unique arc εij𝒜2(S)\varepsilon_{ij}\in\mathcal{A}^{2}(S) such that a1(εij)a^{-1}(\varepsilon_{ij}) is disjoint from both a1(xi)a^{-1}(x_{i}) and a1(xj)a^{-1}(x_{j}), as in Figure 2 (it is the only arc with distinct endpoints in the complement of xixjx_{i}\cup x_{j}).

Refer to caption
Figure 2. The possible configurations for two arcs x0x_{0} and x1x_{1}, and the corresponding arcs ε01\varepsilon_{01}, if needed.

Now by construction, the curves

a1({xi}i=0,1,2{εij}0i<j2)a^{-1}\left(\{x_{i}\}_{i=0,1,2}\cup\{\varepsilon_{ij}\}_{0\leq i<j\leq 2}\right)

form a loop δ\delta in 𝒞S\mathcal{C}S. Therefore we are left to prove that δ\delta can be filled with finitely many pentagons.

If there is a pair of arcs, say, x0x_{0}, x1x_{1}, which have distinct endpoints, then x2x_{2} must share an endpoint with each of them. This shows that δ\delta has precisely 55 vertices, and therefore is filled by a pentagon in 𝒞SP\mathcal{C}S_{P}. Otherwise, suppose that all pairs xix_{i}, xjx_{j} share an endpoint, that is, δ\delta has six vertices. There are five possible cases, as in Figure 3.

Refer to caption
Figure 3. The possible configurations for three arcs x0,x1,x2x_{0},x_{1},x_{2}, and the corresponding arcs εij\varepsilon_{ij}.

Let us analyse all of them separately.

  1. (1)

    The ε\varepsilon-arcs coincide, thus δ=a1({xi}i=0,1,2{ε})\delta=a^{-1}\left(\{x_{i}\}_{i=0,1,2}\cup\{\varepsilon\}\right) is a tripod.

  2. (2)

    Add the arc zz in the Figure. Now {x0,x1,z,ε01,ε12}\{x_{0},x_{1},z,\varepsilon_{01},\varepsilon_{12}\} form a pentagon, as well as {x0,x2,z,ε02,ε12}\{x_{0},x_{2},z,\varepsilon_{02},\varepsilon_{12}\}. Therefore we can fill δ\delta with the preimage under aa of these arcs, which is a union of two pentagons joined along two edges.

  3. (3)

    The ε\varepsilon-arcs coincide, so we are in the same situation as case 1.

  4. (4)

    Similarly to case 2, adding zz creates two pentagons.

  5. (5)

    This time we need four auxiliary curves, in order to form four pentagons P1={x0,a,ε01,ε12,b}P_{1}=\{x_{0},a,\varepsilon_{01},\varepsilon_{12},b\}, P2={x2,a,ε12,ε02,c}P_{2}=\{x_{2},a,\varepsilon_{12},\varepsilon_{02},c\}, P3={x1,a,ε12,d,c}P_{3}=\{x_{1},a,\varepsilon_{12},d,c\} and P4={x1,a,ε01,d,b}P_{4}=\{x_{1},a,\varepsilon_{01},d,b\}.

Now we are ready to prove quasi-isometric rigidity for 𝒞(S0,5)/N\mathcal{C}(S_{0,5})/N:

Theorem 2.8.

Let S=S0,5S=S_{0,5}, and let 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N be a DD-large displacement quotient. If D8D\geq 8 then the map 𝒞𝒢±(S)/NAut(𝒞S/N)\mathcal{MCG}^{\pm}(S)/N\to\text{Aut}(\mathcal{C}S/N) is an isomorphism.

Proof of Theorem 2.8.

Notice first that pentagons in 𝒞S/N\mathcal{C}S/N can be lifted and pentagons in 𝒞S\mathcal{C}S can be projected isometrically, as a consequence of Lemma 1.7. Thus we can consider the quotient 𝒞SP/N\mathcal{C}S_{P}/N, which is again a polygonal complex. Moreover, any automorphism ϕ¯:𝒞S/N𝒞S/N\overline{\phi}:\,\mathcal{C}S/N\to\mathcal{C}S/N maps pentagons to pentagons, and therefore extends to an automorphism of 𝒞SP/N\mathcal{C}S_{P}/N. Now we can argue as in Theorem 2.1, this time using the covering 𝒞SP𝒞SP/N\mathcal{C}S_{P}\to\mathcal{C}S_{P}/N, to show that the map 𝒞𝒢±(S)/NAut(𝒞S/N)\mathcal{MCG}^{\pm}(S)/N\to\text{Aut}(\mathcal{C}S/N) is an isomorphism (again, injectivity follows from [FM12, Section 3.4]). ∎

3. Quasi-isometric rigidity

This section is devoted to the proof of Theorem 2 from the Introduction, that is quasi-isometric rigidity of certain large displacement quotients, which admit a particular hierarchically hyperbolic group (HHG) structure (see Theorem 3.8 for the exact statement). The idea is to show that, from any self-quasi-isometry ff of a HHG satisfying some additional assumptions, one can extract an automorphism of a certain graph, which in our case will coincide with 𝒞S/N\mathcal{C}S/N. Then we will be able to apply the combinatorial rigidity results from Section 2 to produce a candidate element g¯𝒞𝒢±(S)/N\overline{g}\in\mathcal{MCG}^{\pm}(S)/N, and with a little more effort we will show that ff coarsely coincides with the left multiplication by g¯\overline{g}. Once again, I am grateful to Jason Behrstock, Mark Hagen, and Alessandro Sisto for their contribution, in particular to the proof of Lemma 3.15.

3.1. Background on hierarchical hyperbolicity

First, we recall the intuition behind some notions from the world of hierarchically hyperbolic spaces and groups, first introduced by Behrstock, Hagen, and Sisto in [BHS17b]. We refer to [BHS19] for the details of the definitions.

3.1.1. HHS and HHG

A hierarchically hyperbolic space (HHS for short) is a metric space XX that comes with certain additional data, most importantly a family of uniformly hyperbolic spaces {𝒞Y}Y𝔖\{\mathcal{C}Y\}_{Y\in\mathfrak{S}}, called coordinate spaces, and uniformly coarsely Lipschitz maps πY:X𝒞Y\pi_{Y}:X\to\mathcal{C}Y, which shall be thought of as coordinates for points in XX. For mapping class groups, these are curve graphs of subsurfaces and maps coming from subsurface projections. Moreover, the domain set 𝔖\mathfrak{S}, that is, the set which indexes the family of coordinate spaces, has a partial ordering \sqsubseteq, called nesting, with a unique maximal element, and an equivalence relation \bot, called orthogonality. For mapping class groups, these are containment and disjointness of subsurfaces (up to isotopy). When two domains U,VU,V of 𝔖\mathfrak{S} are not \sqsubseteq- nor \bot-related, one says that they are transverse, and one writes UVU\pitchfork V. Finally, whenever U⊥̸VU\not\bot V there is a projection ρVU:𝒞U𝒞V\rho^{U}_{V}:\,\mathcal{C}U\to\mathcal{C}V, which for mapping class group is again defined using subsurface projection.

An action of a finitely generated group GG on a hierarchically hyperbolic space (X,𝔖)(X,\mathfrak{S}) is the data of:

  • an action GXG\circlearrowleft X by isometries;

  • an action G𝔖G\circlearrowleft\mathfrak{S}, preserving nesting and orthogonality;

  • for every gGg\in G and every Y𝔖Y\in\mathfrak{S}, an isometry gY:𝒞Y𝒞g(Y)g_{Y}:\,\mathcal{C}Y\to\mathcal{C}g(Y).

Moreover, one requires that the two actions are compatible, meaning that for every gGg\in G and every non-orthogonal domains U,V𝔖U,V\in\mathfrak{S} the following diagrams commute:

X{X}X{X}𝒞U{\mathcal{C}U}𝒞g(U){\mathcal{C}g(U)}g\scriptstyle{g}πU\scriptstyle{\pi_{U}}πU\scriptstyle{\pi_{U}}gU\scriptstyle{g_{U}}𝒞U{\mathcal{C}U}𝒞g(U){\mathcal{C}g(U)}𝒞V{\mathcal{C}V}𝒞g(V){\mathcal{C}g(V)}gU\scriptstyle{g_{U}}ρVU\scriptstyle{\rho^{U}_{V}}ρg(V)g(U)\scriptstyle{\rho^{g(U)}_{g(V)}}gV\scriptstyle{g_{V}}

We will often slightly abuse notation and drop the subscript for the isometries gUg_{U}. If the action on XX is metrically proper and cobounded, and the action on 𝔖\mathfrak{S} is cofinite, then GG is a hierarchically hyperbolic group (HHG for short), and any quasi-isometry between GG and XX given by the Milnor-Švarc lemma can be used to endow GG with the HHS structure of XX.

For later purposes, we point out that hierarchically hyperbolic groups are examples of asymphoric HHS, in the sense of [BHS21, Definition 1.14], though we will not need the actual definition of this property.

3.1.2. Product, flats, orthants

The idea of orthogonality is that it corresponds to products, in the following sense. Given any U𝔖U\in\mathfrak{S}, there is a corresponding space FUF_{U} associated to it, which is quasi-isometrically embedded in XX (FUF_{U} is a HHS itself with domain set 𝔖U={Y𝔖:YU}\mathfrak{S}_{U}=\{Y\in\mathfrak{S}:Y\sqsubseteq U\}, and in mapping class groups these essentially correspond to mapping class groups of subsurfaces). Given a maximal set {Ui}\{U_{i}\} of pairwise orthogonal elements of 𝔖\mathfrak{S}, there is a corresponding standard product region P{Ui}P_{\{U_{i}\}} which is quasi-isometric to the product of the FUiF_{U_{i}} (think of a Dehn twist flat as, coarsely, a product of annular curve graphs).

Moreover, inside XX and the FUF_{U}s there are special (uniform) quasi-geodesics, called hierarchy paths, which are those that project monotonically (with uniform constants) to all 𝒞Y\mathcal{C}Y. Similarly, there are hierarchy rays and hierarchy lines (which are quasigeodesic rays and lines, respectively). Given a product region P{Ui}P_{\{U_{i}\}} and hierarchy lines (resp., rays) in some of the FUiF_{U_{i}}, the product region contains a product of those (where for the indices ii for which a line/ray has not been assigned one chooses a point in FUiF_{U_{i}} instead). This is what we will refer to as standard kk-flats (resp., orthants), where kk is the number of lines/rays. The support of a standard kk-flat (resp., orthant) is the set of UiU_{i} for which a line/ray has been assigned. Related to this, a complete support set is a subset {Ui}i=1ν𝔖\{U_{i}\}_{i=1}^{\nu}\subseteq\mathfrak{S} of pairwise orthogonal domains with all 𝒞Ui\mathcal{C}U_{i} unbounded, and with maximal possible cardinality ν\nu among sets with these properties. This definition is relevant here as ν\nu, which is called the rank of XX, is then the maximal dimension of standard orthants (if the 𝒞Ui\mathcal{C}U_{i} are not only unbounded, but also have non-empty Gromov boundary, as will be the case for us). Moreover, in this case points in the Gromov boundary C(Ui)\partial C(U_{i}) each determine a hierarchy ray, and similarly pairs of points determine hierarchy lines. In particular, for every complete support set {Ui}i=1ν\{U_{i}\}_{i=1}^{\nu} and for every choice of distinct points pi±𝒞Uip_{i}^{\pm}\in\partial\mathcal{C}U_{i} there exists an associated standard ν\nu-flat 𝔉{(Ui,pi±)}\mathfrak{F}_{\{(U_{i},p_{i}^{\pm})\}}, which is the product of the hierarchy lines in FUiF_{U_{i}} whose projections to 𝒞Ui\mathcal{C}U_{i} have endpoints pi±p_{i}^{\pm}. We will refer to standard ν\nu-flats (resp. standard ν\nu-orthants) simply as standard flats (resp. standard orthants).

The following Lemma, which follows from carefully inspecting the proofs of [BHS21, Lemmas 4.11 and 4.12], describes the (coarse) intersection of standard flats and orthants. Recall that, given subsets A,BA,B of a metric space XX, the coarse intersection A~BA\tilde{\cap}B, if well-defined, is a subspace of XX within bounded Hausdorff distance of all intersections NR(A)NR(B)N_{R}(A)\cap N_{R}(B) of their RR-neighbourhoods, for RR sufficiently large.

Lemma 3.1 (Coarse intersection of standard orthants and flats).

Let (X,𝔖)(X,\mathfrak{S}) be an asymphoric HHS of rank ν\nu.

  • Let 𝒪,𝒪\mathcal{O},\mathcal{O}^{\prime} be standard orthants in XX with supports {Ui}i=1ν\{U_{i}\}_{i=1}^{\nu} and {Vi}i=1ν\{V_{i}\}_{i=1}^{\nu}. Then 𝒪~𝒪\mathcal{O}\tilde{\cap}\mathcal{O}^{\prime} is well-defined, and coarsely coincides with a standard kk–orthant whose support is contained in {Ui}i=1ν{Vi}i=1ν\{U_{i}\}_{i=1}^{\nu}\cap\{V_{i}\}_{i=1}^{\nu}.

  • Let ,\mathcal{F},\mathcal{F}^{\prime} be standard orthants in XX with supports {Ui}i=1ν\{U_{i}\}_{i=1}^{\nu} and {Vi}i=1ν\{V_{i}\}_{i=1}^{\nu}. Then ~\mathcal{F}\tilde{\cap}\mathcal{F}^{\prime} is well-defined, and coarsely coincides with a product TT\prod_{T}\ell_{T}, where TT varies in {Ui}i=1ν{Vi}i=1ν\{U_{i}\}_{i=1}^{\nu}\cap\{V_{i}\}_{i=1}^{\nu} and every T\ell_{T} is either a point, a standard 11-orthant or a standard 11-flat supported on TT.

3.2. HHG structures inherited from the surface

From now on, we will further restrict our attention to those large displacement quotients admitting a HHG structure whose “interesting” domains are orbits of subsurfaces:

Convention 3.2 (Surface-inherited HHG structure).

𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N is a DD-large displacement quotient for some D8D\geq 8, and it admits a HHG structure with the following properties:

  • The domain set is 𝔗=𝔖¯𝔗\mathfrak{T}=\overline{\mathfrak{S}}\sqcup\mathfrak{T}^{\prime}, where 𝔖¯=𝔖/N\overline{\mathfrak{S}}=\mathfrak{S}/N is the collection of NN-orbits of essential subsurfaces.

  • Two domains U¯,V¯𝔖¯\overline{U},\overline{V}\in\overline{\mathfrak{S}} are nested (resp. orthogonal) if and only if they admit representatives U,V𝔖U,V\in\mathfrak{S} which are nested (resp. orthogonal).

  • The \sqsubseteq-maximal element of 𝔗\mathfrak{T} is (the NN-orbit of) the whole surface SS, and its coordinate space, which we refer to as the top-level coordinate space, is 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N-equivariantly quasi-isometric to 𝒞S/N\mathcal{C}S/N. In particular, 𝒞S/N\mathcal{C}S/N is hyperbolic.

  • Whenever U¯𝔖¯\overline{U}\in\overline{\mathfrak{S}} is not the \sqsubseteq-maximal element, the coordinate space associated to U¯\overline{U} is (UU¯𝒞U)/N\left(\bigcup_{U\in\overline{U}}\mathcal{C}U\right)/N. Furthermore, the quotient projection UU¯𝒞U𝒞U¯\bigcup_{U\in\overline{U}}\mathcal{C}U\to\mathcal{C}\overline{U} restricts to a quasi-isometry 𝒞U𝒞U¯\mathcal{C}U\to\mathcal{C}\overline{U}, for any representative UU¯U\in\overline{U}. Here 𝒞U\mathcal{C}U is the usual curve graph of UU, unless UU has complexity 11 and 𝒞U\mathcal{C}U is isomorphic to the Farey complex, or UU is an annulus and 𝒞U\mathcal{C}U is its annular curve graph.

  • There exists a constant EE such that, for every T𝔗T\in\mathfrak{T}^{\prime}, either diam(𝒞T)E\mathrm{diam}(\mathcal{C}T)\leq E or TT is not orthogonal to any other element of 𝔗\mathfrak{T}.

Here are some examples of quotients with a surface-inherited structure.

Example 3.3.

𝒞𝒢±(S)\mathcal{MCG}^{\pm}(S) itself has a HHG structure whose domain set coincides with 𝔖\mathfrak{S} and whose coordinate spaces are curve graphs of subsurfaces (see e.g. [BHS19, Theorem 11.1]).

Example 3.4 (Hierarchically hyperbolically embedded subgroups).

Let HH be a finitely generated subgroup of 𝒞𝒢±(S)\mathcal{MCG}^{\pm}(S) which is hierarchically hyperbolically embedded, as defined in [BHS17a, Definition 6.1] building on the notion of hyperbolically embedded subgroups from [DGO17, Definition 2.1]. Lemma 3.5 describes conditions on a subgroup MHM\leq H ensuring that the quotient by the normal closure of MM satisfies Convention 3.2.

Lemma 3.5.

Let H𝒞𝒢±(S)H\leq\mathcal{MCG}^{\pm}(S) be a finitely generated subgroup which is hierarchically hyperbolically embedded. There exists a finite set FH{1}F\subset H-\{1\} such that, if a normal subgroup MHM\unlhd H avoids FF and H/MH/M is hyperbolic, then the quotient 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N by the normal closure of MM satisfies Convention 3.2.

Proof.

Consider any Cayley graph for HH, with respect to any finite set of generators. As noted in [BHS17a, Remark 6.3], the orbit maps of HH to 𝒞S\mathcal{C}S are quasi-isometric embeddings (actually, the image is also quasi-convex). Hence there exists R0R\geq 0 such that, denoted by B(1,R)B(1,R) the ball of radius RR centred at the identity of HH, if MB(1,R)={1}M\cap B(1,R)=\{1\} then MM acts on 𝒞S\mathcal{C}S with minimum displacement at least 88. This in turn means that, for MM- to act with large minimum displacement, it suffices that it avoids finitely many elements, since balls in a Cayley graph of a finitely generated group are finite.

Now we claim that, if MM avoids a possibly bigger finite set, then its normal closure NN acts on 𝒞S\mathcal{C}S with minimum displacement at least 88 as well. This follows from results of [DGO17] on hyperbolically embedded subgroups, but we can give a proof based on the machinery from [CM22]. There the authors take as input our setting and output a projection complex, which we shall think of as the data of:

  • a graph 𝒫\mathcal{P}, whose vertices correspond in our case to orbits of the form gH(x0)𝒞SgH(x_{0})\subset\mathcal{C}S for all g𝒞𝒢±(S)g\in\mathcal{MCG}^{\pm}(S) and for a fixed basepoint x0𝒞S(0)x_{0}\in\mathcal{C}S^{(0)};

  • a notion of projection between vertices of 𝒫\mathcal{P}, which for us is given by projections onto the quasi-convex subsets gH(x0)𝒞SgH(x_{0})\subset\mathcal{C}S;

  • an action N𝒫N\circlearrowleft\mathcal{P}, such that the stabiliser of gH(x0)gH(x_{0}) is precisely gMg1gMg^{-1} (this follows from [DGO17, Theorem 2.14], where NN is described as an infinite free product of conjugates of MM).

An example of the construction of the projection complex for the case when MM is generated by a pseudo-Anosov mapping class can be found in [CM22, Section 8.1].

Now, for every x𝒞S(0)x\in\mathcal{C}S^{(0)} there exists g𝒞𝒢±(S)g\in\mathcal{MCG}^{\pm}(S) such that the orbit gH(x0)gH(x_{0}) is uniformly close to xx, since g𝒞𝒢±(S)gH=𝒞𝒢±(S)\bigcup_{g\in\mathcal{MCG}^{\pm}(S)}gH=\mathcal{MCG}^{\pm}(S) and the action of 𝒞𝒢±(S)\mathcal{MCG}^{\pm}(S) on the curve graph is cofinite. Now let nN{1}n\in N-\{1\}, and we want to say that d𝒞S(x,nx)8\mathrm{d}_{\mathcal{C}S}(x,nx)\geq 8. Notice that we can think of gH(x0)gH(x_{0}) and ngH(x0)ngH(x_{0}) as vertices of 𝒫\mathcal{P}. Therefore, by [CM22, Proposition 3.2] one of the following must hold:

  • nn fixes gH(x0)gH(x_{0}), and therefore it belongs to gMg1gMg^{-1}. In particular, nn has minimum displacement at least 88, since we already know that every non-trivial element in MM does and minimum displacement is preserved under conjugation.

  • nn fixes ngH(x0)ngH(x_{0}), and for the same reason it has minimum displacement at least 88.

  • There exists a third vertex of 𝒫\mathcal{P}, that is, a third orbit gH(x0)g^{\prime}H(x_{0}), on which gH(x0)gH(x_{0}) and ngH(x0)ngH(x_{0}) have distant projection. Now, the projection of xx is close to the projection of gH(x0)gH(x_{0}), and similarly nxnx projects close to ngH(x0)ngH(x_{0}). Therefore xx and nxnx have distant projections to gH(x0)g^{\prime}H(x_{0}), and in turn this means that xx and nxnx are far from each other in 𝒞S\mathcal{C}S.

Now, [BHS17a, Theorem 6.2] states that, if MM avoids a (possibly larger) finite set and H/MH/M is hyperbolic, then 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N admits a hierarchically hyperbolic structure with the following properties:

  • The index set is 𝔗=𝔖¯{NgH}g𝒞𝒢±(S)\mathfrak{T}=\overline{\mathfrak{S}}\cup\{NgH\}_{g\in\mathcal{MCG}^{\pm}(S)};

  • Orthogonality and nesting in 𝔖¯\overline{\mathfrak{S}} correspond to orthogonality and nesting between representatives;

  • If U¯𝔖¯\overline{U}\in\overline{\mathfrak{S}} is not the maximal element, then 𝒞U¯\mathcal{C}\overline{U} is quasi-isometric to 𝒞U\mathcal{C}U via the projection map, for any representative UU for U¯\overline{U};

  • If T𝔗T\in\mathfrak{T} is of the form NgHNgH then TT has no orthogonal, and 𝒞T\mathcal{C}T is isometric to H/MH/M;

  • The top-level coordinate space is obtained from 𝒞S/N\mathcal{C}S/N after coning off every H/MH/M-orbit.

Thus all requirements of Convention 3.2 are satisfied, except for the quasi-isometry type of the top-level coordinate space. Now one can apply the procedure from [ABD21, Theorem 3.7] to remove the domains without orthogonals, and get a new structure (𝒞𝒢±(S)/N,)(\mathcal{MCG}^{\pm}(S)/N,\mathfrak{R}) such that:

  • The new index set coincides with the maximal element, together with all elements 𝔗\mathfrak{T} admitting an orthogonal domain with unbounded coordinate space. Hence =𝔖¯\mathfrak{R}=\overline{\mathfrak{S}};

  • Orthogonality and nesting are inherited from the original structure;

  • If U¯𝔖¯\overline{U}\in\overline{\mathfrak{S}} is not the maximal element, then 𝒞U¯\mathcal{C}\overline{U} is unchanged;

  • The top-level coordinate space is the space X^\widehat{X} obtained from 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N after coning off the factors FU¯F_{\overline{U}} for every non-maximal U¯𝔖¯\overline{U}\in\overline{\mathfrak{S}}. These factors correspond to the stabilisers of the action of 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N on 𝒞S/N\mathcal{C}S/N. Therefore, by a version of the Milnor-Švarc Lemma described in e.g. [CC07, Theorem 5.1], 𝒞S/N\mathcal{C}S/N is quasi-isometric to X^\widehat{X}.

Therefore the new structure satisfies Convention 3.2. ∎

Now we can finally prove that the quotient by a high enough power of a pseudo-Anosov element is a large displacement quotient:

Corollary 3.6.

Let f𝒞𝒢±(S)f\in\mathcal{MCG}^{\pm}(S) be pseudo-Anosov element. There exists K0K_{0}\in\mathbb{N} such that, if K{0}K\in\mathbb{Z}-\{0\} is a multiple of K0K_{0}, then the quotient 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N by the normal closure of fKf^{K} satisfies Convention 3.2, and in particular is a DD-large displacement for some D8D\geq 8.

Proof.

The elementary closure E(f)E(f) of a pseudo-Anosov element f𝒞𝒢±(S)f\in\mathcal{MCG}^{\pm}(S), that is, the unique maximal virtually-cyclic subgroup containing ff, is hierarchically hyperbolically embedded (this ultimately follows from [DGO17, Theorem 6.50]). Moreover, by inspection of the proof of [DGO17, Lemma 6.5], the cyclic group f\langle f\rangle generated by ff has finite index in E(f)E(f), therefore there exists K0K_{0} such that fK0\langle f^{K_{0}}\rangle is normal in E(f)E(f). We can further assume that fK0\langle f^{K_{0}}\rangle avoids the finite set FE(f)F\subset E(f) given by Lemma 3.5. Hence, the hypothesis of Lemma 3.5 are satisfied by fK\langle f^{K}\rangle whenever KK is a non-trivial multiple of K0K_{0}. ∎

For later purposes, we also notice that the existence of a surface-inherited HHG structure implies that 𝒞/N\mathcal{C}/N is unbounded, though in all known examples this is already true for less artificial reasons:

Lemma 3.7.

Let SS be either a surface of complexity at least 22, and let 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N satisfy Convention 3.2. Then 𝒞S/N\mathcal{C}S/N is unbounded.

Proof.

By [PS23, Theorem 3.2], with holds for any HHG, there exists a maximal family {T1,,Tk}𝔗\{T_{1},\ldots,T_{k}\}\subset\mathfrak{T} of pairwise orthogonal domains with unbounded coordinate spaces, such that any other domain R𝔗R\in\mathfrak{T} with unbounded coordinate space is nested in one of the TiT_{i}. If one of the TiT_{i} is the \sqsubseteq-maximal element then we are done, because then its coordinate space, which by Convention 3.2 is quasi-isometric to 𝒞S/N\mathcal{C}S/N, must be unbounded.

Otherwise, pick an annulus UU, and let VV be the subsurface obtained from SUS-U after removing all connected components which are pants. Since the complexity is at least 22, VV is actually an element of 𝔖\mathfrak{S}, which is nested only inside SS and itself. Moreover, if we denote its NN-orbit by V¯\overline{V}, then 𝒞V¯\mathcal{C}\overline{V} is quasi-isometric to 𝒞V\mathcal{C}V and is therefore unbounded. Thus, without loss of generality V¯T1\overline{V}\sqsubseteq T_{1}, and since T1T_{1} is not the maximal element, we must have that T1=V¯T_{1}=\overline{V}. In particular, since any other TiT_{i} is orthogonal to T1T_{1}, the collection {T1,,Tk}\{T_{1},\ldots,T_{k}\} can consist only of V¯\overline{V} and U¯\overline{U}.

Now it is enough to produce an annulus WW whose NN-orbit W¯\overline{W} is not nested in either V¯\overline{V} or U¯\overline{U}, and this will lead to a contradiction because 𝒞W¯\mathcal{C}\overline{W} is unbounded by our Convention. Let xx be the core of UU, which is also the boundary of VV inside SS, pick a curve y𝒞S(0)y\in\mathcal{C}S^{(0)} at distance 22 from xx, and let WW be the annulus with core yy. Then all NN-translates of xx must be at distance at least 22 from yy, by the assumption on the minimum displacement, and this means that all NN-translates of WW must cross UU. In particular W¯\overline{W} cannot be nested in either U¯\overline{U} or V¯\overline{V}. ∎

3.3. Statement of the results

The goal of this Section is to prove that, if 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N satisfies Convention 3.2, then it is quasi-isometrically rigid in the following sense. Recall that two groups GG and HH are said to be weakly commensurable if there exist two finite normal subgroups LHL\unlhd H and MGM\unlhd G such that the quotients H/LH/L and G/MG/M have two finite index subgroups that are isomorphic.

Theorem 3.8 (Quasi-isometric rigidity).

Let SS be a surface of complexity at least 22 which is not a torus with two punctures, and let 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N satisfy Convention 3.2. Then MCG/NMCG/N is quasi-isometrically rigid, meaning that if a finitely generated group GG and 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N are quasi-isometric then they are weakly commensurable.

As we will see, the assumption on the topological type of SS is needed to ensure that every automorphism of 𝒞S/N\mathcal{C}S/N is induced by a mapping class, as a consequence of Theorems 2.1, 2.4 and 2.8. Moreover, we require the complexity to be at least 22, so that in 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N we can find “Dehn Twist flats”, that is, standard flats supported on the orbits of pairwise disjoint annuli, of dimension at least 22. See Lemma 3.20 for more details.

Since 𝒞𝒢±(S)\mathcal{MCG}^{\pm}(S) itself is a DD-large displacement quotient for every choice of DD, as pointed out in Example 1.3, we also recover quasi-isometric rigidity of mapping class groups:

Corollary 3.9 (QI-rigidity of 𝒞𝒢±(S)\mathcal{MCG}^{\pm}(S)).

Let SS be a surface of complexity at least 22 which is not a torus with two punctures. Then 𝒞𝒢±(S)\mathcal{MCG}^{\pm}(S) is quasi-isometrically rigid, meaning that if a finitely generated group GG and 𝒞𝒢±(S)\mathcal{MCG}^{\pm}(S) are quasi-isometric then they are weakly commensurable.

Moreover, in view of Lemma 3.5 we get the following:

Corollary 3.10.

Let SS be a surface of complexity at least 22 which is not a torus with two punctures. Let H𝒞𝒢±(S)H\leq\mathcal{MCG}^{\pm}(S) be a hierarchically hyperbolically embedded subgroup, let MHM\leq H and let NN be the normal closure of MM. There exists a finite set FH{1}F\subset H-\{1\} such that, if MM avoids FF and H/MH/M is hyperbolic, then 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N is quasi-isometrically rigid, meaning that if a finitely generated group GG and 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N are quasi-isometric then they are weakly commensurable.

3.4. Quasi-isometries induce maps on hinges

For this Subsection only, we will work in the general framework of an asymphoric HHS (X,𝔖)(X,\mathfrak{S}) of rank ν\nu. We will show that, if XX satisfies some additional properties (see Assumptions (A) - (F)), then any self-quasi-isometry of XX induces an automorphism of a certain graph, which we shall think of as encoding certain standard flats and their intersections.

Recall that a complete support set is a collection {U1}i=1ν𝔖\{U_{1}\}_{i=1}^{\nu}\subset\mathfrak{S} of pairwise orthogonal domains with unbounded coordinate spaces, with maximal cardinality ν\nu among all such collections.

Definition 3.11 ([BHS21, Definition 5.2]).

A hinge is a pair (U,p)(U,p) where UU belongs to a complete support set and pCUp\in\partial CU. We say that UU is the support of (U,p)(U,p). Let 𝐇𝐢𝐧𝐠𝐞(𝔖)\bf{Hinge}(\mathfrak{S}) be the set of hinges.

As in [BHS21, Definition 5.3], one can associate to a hinge σ=(U,p)\sigma=(U,p) a standard 11-orthant, denoted 𝔥σ\mathfrak{h}_{\sigma}. This is a hierarchy ray whose projection to 𝒞U\mathcal{C}U is a quasigeodesic ray asymptotic to pp, and whose projections to all other coordinate spaces are uniformly bounded. Another property of 𝔥σ\mathfrak{h}_{\sigma}, stated in [BHS21, Remark 5.4], is that if σσ\sigma\neq\sigma^{\prime} are two different hinges then dHaus(𝔥σ,𝔥σ)=\mathrm{d}_{Haus}(\mathfrak{h}_{\sigma},\mathfrak{h}_{\sigma^{\prime}})=\infty.

Let us introduce the first set of hypothesis on (X,𝔖)(X,\mathfrak{S}).

Assumption A.

For every UU which belongs to a complete support set, the Gromov boundary 𝒞U\partial\mathcal{C}U of its coordinate space consists of at least 22 points.

Definition 3.12 (Good domain).

A domain U𝔖U\in\mathfrak{S} is good if there exist two complete support sets whose intersection is {U}\{U\}. Let 𝔖G\mathfrak{S}_{G} be the set of good domains, and let 𝐇𝐢𝐧𝐠𝐞G(𝔖)\mathbf{Hinge}_{G}(\mathfrak{S}) be the set of hinges supported on good domains.

Assumption B.

For every U,V𝔖GU,V\in\mathfrak{S}_{G} which are orthogonal, there exist two support sets whose intersection is {U,V}\{U,V\}.

Assumption C.

For every U𝔖U\in\mathfrak{S} which belongs to a complete support set, there exists a (possibly empty) collection of good domains {V1,,Vn}\{V_{1},\ldots,V_{n}\} and two complete support sets whose intersection is {U,V1,,Vn}\{U,V_{1},\ldots,V_{n}\}.

Remark 3.13.

Let f:XXf:\,X\to X be a quasi-isometry. With the same arguments as in the first half of the proof of [BHS21, Theorem 5.7], one can define a map fHin:𝐇𝐢𝐧𝐠𝐞G(𝔖)𝐇𝐢𝐧𝐠𝐞(𝔖)f_{Hin}:\,\mathbf{Hinge}_{G}(\mathfrak{S})\to\mathbf{Hinge}(\mathfrak{S}) by mapping σ𝐇𝐢𝐧𝐠𝐞G(𝔖)\sigma\in\mathbf{Hinge}_{G}(\mathfrak{S}) to the unique hinge σ𝐇𝐢𝐧𝐠𝐞(𝔖)\sigma^{\prime}\in\mathbf{Hinge}(\mathfrak{S}) such that dHaus(f(𝔥σ),𝔥σ)<+\mathrm{d}_{\text{Haus}}(f(\mathfrak{h}_{\sigma}),\mathfrak{h}_{\sigma^{\prime}})<+\infty. Moreover, by inspection of the construction one sees that σ\sigma^{\prime} is itself good, since 𝔥σ\mathfrak{h}_{\sigma^{\prime}} arises as the coarse intersection of two standard orthants (whose supports must therefore coincide only on the support of σ\sigma^{\prime} by Lemma 3.1). Hence fHinf_{Hin} maps 𝐇𝐢𝐧𝐠𝐞G(𝔖)\mathbf{Hinge}_{G}(\mathfrak{S}) to itself, and therefore is a bijection whose inverse is the map gHing_{Hin}, induced by any quasi-inverse gg for ff.

Definition 3.14.

We say that two hinges are co-supported if they are supported on the same domain, i.e. if the union of their hinge rays is (coarsely) a 1-dimensional standard flat. We say that two hinges are orthogonal if they are supported on orthogonal domains.

Lemma 3.15 (Behrstock, Hagen, Sisto).

Under Assumptions (A) - (C), if two good hinges σ,σ𝐇𝐢𝐧𝐠𝐞G(𝔖)\sigma,\sigma^{\prime}\in\mathbf{Hinge}_{G}(\mathfrak{S}) are orthogonal then fHin(σ)f_{Hin}(\sigma) and fHin(σ)f_{Hin}(\sigma^{\prime}) are either orthogonal or co-supported.

Proof.

Let σ=(U,p)\sigma=(U,p) and σ=(U,p)\sigma^{\prime}=(U^{\prime},p^{\prime}). By Assumption (B) there exist two standard flats 1,2\mathcal{F}_{1},\mathcal{F}_{2} whose coarse intersection is a standard 2-flat containing 𝔥σ\mathfrak{h}_{\sigma} and 𝔥σ\mathfrak{h}_{\sigma^{\prime}}. Let 𝒪\mathcal{O} be the orthant spanned by 𝔥σ\mathfrak{h}_{\sigma} and 𝔥σ\mathfrak{h}_{\sigma^{\prime}} in this standard 2-flat.

As a consequence of the Quasiflats Theorem [BHS21, Theorem A] and of Lemma 3.1, f(1)~f(2)f(\mathcal{F}_{1})\tilde{\cap}f(\mathcal{F}_{2}) is a union of standard 2-orthants, whose “boundary” 1-orthants, which we call coordinate rays, can be ordered cyclically. Moreover, f(𝔥σ)f(\mathfrak{h}_{\sigma}) must arise as some coordinate ray, since it coarsely coincides with some hinge 𝔥fHin(σ)\mathfrak{h}_{f_{Hin}(\sigma)}, and if a hinge is contained in a standard 2-orthant then it must be one of its boundary 1-orthants by [BHS21, Lemma 4.11]. The same is true for f(𝔥σ)f(\mathfrak{h}_{\sigma^{\prime}}).

Now, if f(𝔥σ)f(\mathfrak{h}_{\sigma}) and f(𝔥σ)f(\mathfrak{h}_{\sigma^{\prime}}) are adjacent in the cyclic ordering, then they belong to a common 2-orthant, and therefore they are orthogonal. Thus suppose that there is a coordinate ray rf(𝒪)r\in f(\mathcal{O}) between f(𝔥σ)f(\mathfrak{h}_{\sigma}) and f(𝔥σ)f(\mathfrak{h}_{\sigma^{\prime}}), and let V𝔖V\in\mathfrak{S} be its support.

If VV is good then we can proceed as in the proof of [BHS21, Theorem 5.7] to get a contradiction. Indeed, in this case f1(r)f^{-1}(r) must coincide with some hinge ray 𝔥σ′′\mathfrak{h}_{\sigma^{\prime\prime}}, which belongs to 𝒪\mathcal{O} but lies at infinite Hausdorff distance from both 𝔥σ\mathfrak{h}_{\sigma} and 𝔥σ\mathfrak{h}_{\sigma^{\prime}}, and this contradicts [BHS21, Lemma 4.11].

Then we can assume that no ray between f(𝔥σ)f(\mathfrak{h}_{\sigma}) and f(𝔥σ)f(\mathfrak{h}_{\sigma^{\prime}}) is supported on a good domain, and in particular that VV is not good. By Assumption (C) there exists a collection of good domains {V1,,Vn}\{V_{1},\ldots,V_{n}\} and two complete support sets whose intersection is {V,V1,,Vn}\{V,V_{1},\ldots,V_{n}\}.

Hence, there exist two standard flats 𝒢1,𝒢2\mathcal{G}_{1},\mathcal{G}_{2} whose intersection is a flat supported on {V,V1,,Vn}\{V,V_{1},\ldots,V_{n}\} and containing rr. Now consider Y=𝒢1~𝒢2~f(1)~f(2)Y=\mathcal{G}_{1}\tilde{\cap}\mathcal{G}_{2}\tilde{\cap}f(\mathcal{F}_{1})\tilde{\cap}f(\mathcal{F}_{2}). This coarse intersection is well-defined, since both f(1)f(\mathcal{F}_{1}) and f(2)f(\mathcal{F}_{2}) are finite unions of standard orthants by the Quasiflat Theorem, and the coarse intersection of standard orthants and flats is well-defined by Lemma 3.1. Moreover, let Z=f1(Y)Z=f^{-1}(Y), which is a union of standard 1- and 2-orthants supported on {U,U}\{U,U^{\prime}\} (again, this follows from combining the Quasiflat Theorem, applied to f1(𝒢1)f^{-1}(\mathcal{G}_{1}) and f1(𝒢2)f^{-1}(\mathcal{G}_{2}), and Lemma 3.1). Now, ZZ contains the ray f1(r)f^{-1}(r), which lies inside 𝒪\mathcal{O} but cannot coarsely coincide with 𝔥σ\mathfrak{h}_{\sigma} nor with 𝔥σ\mathfrak{h}_{\sigma^{\prime}}, since their image lie at infinite Hausdorff distance. Therefore, ZZ must contain the whole 2-orthant 𝒪\mathcal{O}. In turn, this means that YY must contain all 2-orthants of f(1)~f(2)f(\mathcal{F}_{1})\tilde{\cap}f(\mathcal{F}_{2}) which lie between f(𝔥σ)f(\mathfrak{h}_{\sigma}) and f(𝔥σ)f(\mathfrak{h}_{\sigma^{\prime}}) in the cyclic ordering, and moreover the support of every such 2-orthant must be contained in {V,V1,,Vn}\{V,V_{1},\ldots,V_{n}\}.

Now, since f(𝔥σ)f(\mathfrak{h}_{\sigma}) and f(𝔥σ)f(\mathfrak{h}_{\sigma^{\prime}}) are boundary 1-orthants of some 2-orthants of YY, their supports must belong to {V,V1,,Vn}\{V,V_{1},\ldots,V_{n}\}, and therefore they are either orthogonal or co-supported. ∎

For the rest of the Section, we will work under the following additional assumptions:

Assumption D.

If U𝔖GU\in\mathfrak{S}_{G} is a good domain, then |𝒞U|=2|\partial\mathcal{C}U|=2.

Assumption E.

For every two good domains UV𝔖GU\neq V\in\mathfrak{S}_{G} there exists a good domain W𝔖GW\in\mathfrak{S}_{G} which is orthogonal to UU but not to VV. In other words, every good domain is uniquely determined by the set of good domains which are orthogonal to it.

Lemma 3.16.

Under Assumptions (A) - (E), if σ,σ𝐇𝐢𝐧𝐠𝐞G(𝔖)\sigma,\sigma^{\prime}\in\mathbf{Hinge}_{G}(\mathfrak{S}) are co-supported then fHin(σ)f_{Hin}(\sigma) and fHin(σ)f_{Hin}(\sigma^{\prime}) are either orthogonal or co-supported.

Proof.

Let σ,σ𝐇𝐢𝐧𝐠𝐞G(𝔖)\sigma,\sigma^{\prime}\in\mathbf{Hinge}_{G}(\mathfrak{S}) be two co-supported good hinges. For every good hinge θ\theta which is orthogonal to fHin(σ)f_{Hin}(\sigma) we can consider its preimage (fHin)1(θ)(f_{Hin})^{-1}(\theta). By Lemma 3.15, which also applies to (fHin)1(f_{Hin})^{-1} (again, because it coincides with the map gHing_{Hin} for any quasi-inverse gg for ff), we have that (fHin)1(θ)(f_{Hin})^{-1}(\theta) and σ\sigma are either orthogonal or co-supported. Moreover, by Assumption (D) the unique hinge which has the same support of σ\sigma is σ\sigma^{\prime}, thus (fHin)1(θ)(f_{Hin})^{-1}(\theta) is orthogonal to σ\sigma and therefore also to σ\sigma^{\prime}. Then again Lemma 3.15 tells us that θ\theta and fHin(σ)f_{Hin}(\sigma^{\prime}) are either co-supported or orthogonal.

We can repeat the argument for every good hinge θ\theta which is orthogonal to fHin(σ)f_{Hin}(\sigma), and we get that either fHin(σ)f_{Hin}(\sigma^{\prime}) has the same support of some θ\theta, and therefore is orthogonal to fHin(σ)f_{Hin}(\sigma), or fHin(σ)f_{Hin}(\sigma) and fHin(σ)f_{Hin}(\sigma^{\prime}) are orthogonal to the same hinges, and therefore they are co-supported by Assumption (E). ∎

To conclude the proof, we also need good domains to satisfy the following strengthening of Definition 3.12, which roughly says that good hinges arise as intersection of “good” standard orthants:

Definition 3.17 (Very good domain).

A domain U𝔖U\in\mathfrak{S} is very good if there exist two complete support sets, made of good domains, whose intersection is {U}\{U\}.

Assumption F.

Good domains are very good.

Lemma 3.18.

Under Assumptions (A) - (F), fHinf_{Hin} induces an automorphism fGf_{G} of the graph (𝔖G,)(\mathfrak{S}_{G},\bot), whose vertex set is 𝔖G\mathfrak{S}_{G} and where adjacency corresponds to orthogonality.

Proof.

We can give 𝐇𝐢𝐧𝐠𝐞G(𝔖)\mathbf{Hinge}_{G}(\mathfrak{S}) a simplicial graph structure, by saying that two hinges are adjacent if and only if they are orthogonal or co-supported. Combining Remark 3.13, Lemma 3.15, and Lemma 3.16, we obtain that ff induces a simplicial automorphism of 𝐇𝐢𝐧𝐠𝐞G(𝔖)\mathbf{Hinge}_{G}(\mathfrak{S}). With a slight abuse of notation, we will keep denoting such automorphism as fHinf_{Hin}, since at the level of vertices it maps every good hinge σ\sigma to fHin(σ)f_{Hin}(\sigma).

Now notice that any maximal clique of 𝐇𝐢𝐧𝐠𝐞G(𝔖)\mathbf{Hinge}_{G}(\mathfrak{S}) is the (infinite) subgraph spanned by all hinges supported on some complete support set, made of good domains. Moreover, we claim that two good hinges σ\sigma and σ\sigma^{\prime} are co-supported if and only if they belong to the same maximal cliques. Indeed, if two hinges are co-supported then they clearly belong to the same maximal cliques; conversely, if σ\sigma and σ\sigma^{\prime} are supported on UVU\neq V, respectively, then one of the following holds:

  • UVU\pitchfork V, and therefore σ\sigma and σ\sigma^{\prime} cannot belong to the same maximal cliques since they are not adjacent in 𝐇𝐢𝐧𝐠𝐞G(𝔖)\mathbf{Hinge}_{G}(\mathfrak{S});

  • UVU\bot V, and in view of Assumption (F) we can find a complete support set, made of good domains, which contains UU but not VV.

Since we just showed that being co-supported is a purely combinatorial property, it must be preserved by the automorphism fHinf_{Hin}. Moreover, the same argument works for the inverse (fHin)1(f_{Hin})^{-1}, hence two good hinges σ,σ𝐇𝐢𝐧𝐠𝐞G(𝔖)\sigma,\sigma^{\prime}\in\mathbf{Hinge}_{G}(\mathfrak{S}) are co-supported if and only if fHin(σ)f_{Hin}(\sigma) and fHin(σ)f_{Hin}(\sigma^{\prime}) are co-supported. This also implies that two good hinges σ,σ𝐇𝐢𝐧𝐠𝐞G(𝔖)\sigma,\sigma^{\prime}\in\mathbf{Hinge}_{G}(\mathfrak{S}) are orthogonal if and only if fHin(σ)f_{Hin}(\sigma) and fHin(σ)f_{Hin}(\sigma^{\prime}) are orthogonal.

Now, fHinf_{Hin} induces an automorphism fGf_{G} of (𝔖G,)(\mathfrak{S}_{G},\bot) as follows. For every U𝔖U\in\mathfrak{S} choose a hinge σ\sigma supported on UU, and set fG(U)f_{G}(U) as the support of fHin(σ)f_{Hin}(\sigma). This map is well-defined since fHinf_{Hin} maps co-supported hinges to co-supported hinges, and it preserves orthogonality since fHinf_{Hin} does. ∎

The last Lemma gives a uniform bound between the image of a maximal flat, supported on good domains, and the maximal flat supported on the image of the supports. In the case of 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N, this will tell us that the quasi-isometry permutes “Dehn twist flats”, up to uniformly bounded distance.

Lemma 3.19 (Flats go to flats).

Let (X,𝔖)(X,\mathfrak{S}) be an asymphoric HHS of rank ν\nu, satisfying Assumptions (A) - (F). For every L0L\geq 0 there exists C0C\geq 0 such that the following holds. Let f:XXf:\,X\to X be a (L,L)(L,L)-quasi-isometry. Let {Ui}i=1ν\{U_{i}\}_{i=1}^{\nu} be a complete support set, made of good domains, and let {Ui}\mathcal{F}_{\{U_{i}\}} be the standard flat it supports. Similarly, let {fG(Ui)}\mathcal{F}_{\{f_{G}(U_{i})\}} the standard flat supported on {fG(Ui)}i=1ν\{f_{G}(U_{i})\}_{i=1}^{\nu}. Then dHaus(f({Ui}),{fG(Ui)})C\mathrm{d}_{Haus}\left(f\left(\mathcal{F}_{\{U_{i}\}}\right),\mathcal{F}_{\{f_{G}(U_{i})\}}\right)\leq C.

Proof.

One can argue as in [BHS21, Lemma 5.9], whose proof only relies on asymphoricity of XX and the fact that fHinf_{Hin} maps hinges on the same support to hinges on the same support. ∎

3.5. Application to large displacement quotients

Now let SS be a surface of complexity at least 22. It is easy to see that, if U𝔖U\in\mathfrak{S} belongs to a complete support set for 𝒞𝒢±(S)\mathcal{MCG}^{\pm}(S), then UU is either an annulus, a S0,4S_{0,4} or a S1,1S_{1,1}. Moreover, if UU has complexity one then every complete support set containing UU must also contain all its boundary annuli, thus UU is not good; on the other hand, annuli are very good, since every annulus can be obtained as intersection of two pants decompositions, that is, two collections of pairwise disjoint annuli. Finally, the rank of 𝒞𝒢±(S)\mathcal{MCG}^{\pm}(S) is precisely the complexity of SS.

The next lemma shows that, if 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N satisfies Convention 3.2, then it fits the framework of Subsection 3.4:

Lemma 3.20.

Let SS be a surface of complexity at least 22, and let 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N satisfy Convention 3.2. Then good domains correspond to NN-orbits of annuli, and Assumptions (A) - (F) hold.

Proof.

First, let {Ui}i=1ζ(S)\{U_{i}\}_{i=1}^{\zeta(S)} be a complete support set for 𝒞𝒢±(S)\mathcal{MCG}^{\pm}(S). The set of all curves lying on i=1ζ(S)Ui\bigcup_{i=1}^{\zeta(S)}U_{i} has diameter at most 22 inside 𝒞S\mathcal{C}S, hence the subsurfaces must belong to pairwise distinct orbits {U¯i}i=1ζ(S)\{\overline{U}_{i}\}_{i=1}^{\zeta(S)} by the assumption on the minimum displacement. Moreover, {U¯i}i=1ζ(S)\{\overline{U}_{i}\}_{i=1}^{\zeta(S)} are again pairwise orthogonal, by how orthogonality in 𝔗\mathfrak{T} is defined, and have unbounded coordinate spaces, since by assumption 𝒞U¯i\mathcal{C}\overline{U}_{i} is quasi-isometric to 𝒞Ui\mathcal{C}U_{i}. Hence the projection of a complete support set for 𝒞𝒢±(S)\mathcal{MCG}^{\pm}(S) is a support set for 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N with the same number of domains, and in particular the rank ν\nu of 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N is at least ζ(S){\zeta(S)}.

Conversely, let 𝒯={T1,,Tν}𝔗\mathcal{T}=\{T_{1},\ldots,T_{\nu}\}\subset\mathfrak{T} be a complete support set. If Ti𝒯T_{i}\in\mathcal{T} belonged to 𝔗𝔖¯\mathfrak{T}-\overline{\mathfrak{S}} then 𝒯\mathcal{T} would only consist of TiT_{i}, because elements of 𝔗𝔖¯\mathfrak{T}-\overline{\mathfrak{S}} with unbounded coordinate spaces have no orthogonals by Convention 3.2. Then 𝒯\mathcal{T} could not be complete, since νζ(S)2\nu\geq{\zeta(S)}\geq 2. Hence, for every i=1,,νi=1,\ldots,\nu, we have that Ti=U¯iT_{i}=\overline{U}_{i}, and by Lemma 1.10 we can find pairwise disjoint representatives UiU¯iU_{i}\in\overline{U}_{i}. Thus ν\nu is at most ζ(S)\zeta(S), and if we combine this with the previous inequality we get ν=ζ(S)\nu=\zeta(S). We just proved that every complete support set for 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N is of the form {U¯i}i=1ζ(S)\{\overline{U}_{i}\}_{i=1}^{\zeta(S)}, for some complete support set {Ui}i=1ζ(S)\{U_{i}\}_{i=1}^{\zeta(S)} for 𝒞𝒢±(S)\mathcal{MCG}^{\pm}(S).

Now, we claim that U¯𝔖¯\overline{U}\in\overline{\mathfrak{S}} is a good domain if and only if it is the orbit of an annulus. Indeed, if U¯\overline{U} is the orbit of an annulus UU we can find two pants decompositions 𝒰\mathcal{U} and 𝒱\mathcal{V} whose intersection is {U}\{U\}. Since all curves in 𝒰𝒱\mathcal{U}\cup\mathcal{V} lie in the ball of radius 11 centred at UU inside 𝒞S\mathcal{C}S, the assumption on the large displacement implies that any two domains in 𝒰𝒱\mathcal{U}\cup\mathcal{V} lie in different NN-orbits. Hence 𝒰¯𝒱¯={U¯}\overline{\mathcal{U}}\cap\overline{\mathcal{V}}=\{\overline{U}\}. On the other hand, if U¯\overline{U} is the class of a subsurface UU of complexity one, then every complete support set 𝒰¯\overline{\mathcal{U}} containing U¯\overline{U} lifts to a complete support set containing UU, which must also contain the boundary annuli of UU. Hence 𝒰¯\overline{\mathcal{U}} must contain the NN-orbit of the boundary annuli of UU.

We conclude the proof by checking the Assumptions:

(A) Whenever U¯\overline{U} belongs to a complete support set, 𝒞U¯\mathcal{C}\overline{U} is isometric to 𝒞U\mathcal{C}U for any of its representatives UU, and in particular has at least two points at infinity.

(B) For every two U¯\overline{U}, V¯\overline{V} which lift to disjoint annuli U,VU,V, we can find two pants decompositions 𝒰\mathcal{U} and 𝒱\mathcal{V} whose intersection is {U,V}\{U,V\}. Moreover, any two annuli in 𝒰𝒱\mathcal{U}\cup\mathcal{V} belong to different NN-orbits, because their core curves are disjoint, so {U¯,V¯}\{\overline{U},\overline{V}\} is the intersection of 𝒰¯\overline{\mathcal{U}} and 𝒱¯\overline{\mathcal{V}}.

(C) Let U¯\overline{U} belong to a complete support set. If U¯\overline{U} is not good, we can pick one of its lift UU and find two complete support sets 𝒰\mathcal{U} and 𝒱\mathcal{V} whose intersection is {U,V1,,Vn}\{U,V_{1},\ldots,V_{n}\}, where {V1,,Vn}\{V_{1},\ldots,V_{n}\} are the boundary annuli of UU. Now, all curves in 𝒰𝒱\mathcal{U}\cup\mathcal{V} lie in the ball of radius 11 centred at any curve xx which lies in UU. Therefore, by the assumption on the large displacement, any two domains in 𝒰𝒱\mathcal{U}\cup\mathcal{V} must belong to different NN-orbits, and in turn this means that {U¯,V¯1,,V¯n}\{\overline{U},\overline{V}_{1},\ldots,\overline{V}_{n}\} is the intersection of 𝒰¯\overline{\mathcal{U}} and 𝒱¯\overline{\mathcal{V}}.

(D) If U¯\overline{U} is good then 𝒞U¯\mathcal{C}\overline{U} is quasi-isometric to an annular curve graph, hence |𝒞U¯|=2|\partial\mathcal{C}\overline{U}|=2.

(E) It is enough to prove that, if x¯,y¯𝒞S/N(0)\overline{x},\overline{y}\in\mathcal{C}S/N^{(0)} have the same link inside 𝒞S/N\mathcal{C}S/N, i.e., if they are adjacent to the same vertices, then they coincide. Indeed, the subgraph spanned by {x¯,y¯}Lk𝒞S/N(x¯)\{\overline{x},\overline{y}\}\cup\text{Lk}_{\mathcal{C}S/N}(\overline{x}) has diameter at most 22, and therefore can be lifted by Lemma 3.16. Thus we get two lifts x,yx,y such that Lk𝒞S(x)\text{Lk}_{\mathcal{C}S}(x) is the lift of Lk𝒞S/N(x¯)\text{Lk}_{\mathcal{C}S/N}(\overline{x}), and therefore coincides with Lk𝒞S(y)\text{Lk}_{\mathcal{C}S}(y). Now we are left to prove that, if two curves x,yx,y have the same link in 𝒞S\mathcal{C}S, then they must coincide. Now, if the curves are disjoint then xLk(y)Lk(x)x\in\text{Lk}(y)-\text{Lk}(x), and we are done. Otherwise, let SS^{\prime} be a component of SxS-{x} which is not a pair of pants (here we are using that SS has complexity at least 22), and let zz be the subsurface projection of yy inside SS^{\prime}. By applying a partial pseudo-Anosov of SS^{\prime} to zz we can find a curve zz^{\prime} inside SS which crosses zz, and therefore also yy.

(F) As we saw before, every U¯\overline{U} which is the orbit of an annulus arises as the intersection of two complete support sets which come from two pants decompositions. Therefore good domains are very good. ∎

Now, good domains correspond to orbits of annuli, and orthogonality corresponds to having disjoint representatives. Hence, as a consequence of Lemma 3.18 we get:

Corollary 3.21.

Let SS be a surface of complexity at least 22, and let 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N satisfy Convention 3.2. Every quasi-isometry f:𝒞𝒢/N𝒞𝒢/Nf:\,\mathcal{MCG}/N\mapsto\mathcal{MCG}/N induces an automorphism f𝒞S/Nf_{\mathcal{C}S/N} of 𝒞S/N\mathcal{C}S/N.

Now we are finally ready to prove quasi-isometric rigidity:

Proof of Theorem 3.8.

Let SS be a surface of complexity at least 22 which is not a S1,2S_{1,2}, and let 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N satisfy Convention 3.2. By [MS23, Lemma 9.15], which follows from standard arguments (see e.g. [Sch95, Section 10.4]), to prove quasi-isometric rigidity of 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N it is enough to verify that, for every L0L\geq 0, there exists R0R\geq 0 such that:

  1. (a)

    Every (L,L)(L,L)-self-quasi-isometry of 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N lies within distance RR from the left multiplication by some element of 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N;

  2. (b)

    If a (L,L)(L,L)-self-quasi-isometry of 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N lies within finite distance from the identity, then it lies within distance RR from the identity.

a Let f:𝒞𝒢±(S)/N𝒞𝒢±(S)/Nf:\,\mathcal{MCG}^{\pm}(S)/N\to\mathcal{MCG}^{\pm}(S)/N be a (L,L)(L,L)-quasi-isometry, and let f𝒞S/Nf_{\mathcal{C}S/N} be the induced automorphism of 𝒞S/N\mathcal{C}S/N. By either Theorem 2.1, Theorem 2.4 or Theorem 2.8, according to the homeomorphism type of SS, we get that f𝒞S/Nf_{\mathcal{C}S/N} is induced by some element g¯𝒞𝒢±(S)/N\overline{g}\in\mathcal{MCG}^{\pm}(S)/N. Moreover, by Lemma 3.19 there exist a constant CC such that, whenever {U¯i}i=1ν\{\overline{U}_{i}\}_{i=1}^{\nu} is a maximal collection of pairwise orthogonal orbits of annuli, ff maps the standard flat {U¯i}\mathcal{F}_{\{\overline{U}_{i}\}} within Hausdorff distance at most CC from {f𝒞S/N(U¯i)}={g¯(U¯i)}\mathcal{F}_{\{f_{\mathcal{C}S/N}(\overline{U}_{i})\}}=\mathcal{F}_{\{\overline{g}(\overline{U}_{i})\}}, which in turn is within Hausdorff distance at most CC from g¯({U¯i})\overline{g}\left(\mathcal{F}_{\{\overline{U}_{i}\}}\right). Therefore dHaus(f({U¯i}),g¯({U¯i}))2C\mathrm{d}_{Haus}\left(f(\mathcal{F}_{\{\overline{U}_{i}\}}),\overline{g}(\mathcal{F}_{\{\overline{U}_{i}\}})\right)\leq 2C.

Now, to show that ff and g¯\overline{g} uniformly coarsely coincide it is enough to say that, for every point x𝒞𝒢±(S)/Nx\in\mathcal{MCG}^{\pm}(S)/N, there exist two standard flats ,\mathcal{F},\mathcal{F}^{\prime}, supported on orbits of annuli, whose coarse intersection is within finite Hausdorff distance from xx, and all constants do not depend on xx. Indeed, if this is the case then ff and g¯\overline{g} should uniformly coarsely agree on the coarse intersection ~\mathcal{F}\tilde{\cap}\mathcal{F}^{\prime}, and therefore on xx. In turn, since 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N acts transitively on itself and maps orbits of annuli to orbits of annuli, it is enough to exhibit a pair ,\mathcal{F},\mathcal{F}^{\prime} of standard flats, supported on orbits of annuli, whose coarse intersection is bounded.

As a consequence of Lemma 3.1, if \mathcal{F} is supported on {U¯i}i=1ν\{\overline{U}_{i}\}_{i=1}^{\nu}, \mathcal{F}^{\prime} is supported on {V¯i}i=1ν\{\overline{V}_{i}\}_{i=1}^{\nu}, and {U¯i}i=1ν{V¯i}i=1ν=\{\overline{U}_{i}\}_{i=1}^{\nu}\cap\{\overline{V}_{i}\}_{i=1}^{\nu}=\emptyset, then the coarse intersection is bounded. Thus, we are left to find two collections {U¯i}i=1ν\{\overline{U}_{i}\}_{i=1}^{\nu} and {V¯i}i=1ν\{\overline{V}_{i}\}_{i=1}^{\nu} of pairwise orthogonal orbits of annuli whose intersection is empty. By Lemma 1.7, it is enough to find two pants decompositions {Ui}i=1ν\{U_{i}\}_{i=1}^{\nu} and {Vi}i=1ν\{V_{i}\}_{i=1}^{\nu} such that {Ui}i=1ν{Vi}i=1ν=\{U_{i}\}_{i=1}^{\nu}\cap\{V_{i}\}_{i=1}^{\nu}=\emptyset and the subgraph of 𝒞S\mathcal{C}S spanned by the core curves of {Ui}i=1ν{Vi}i=1ν\{U_{i}\}_{i=1}^{\nu}\cup\{V_{i}\}_{i=1}^{\nu} has diameter at most 22. This is easy: just pick any pants decomposition {Ui}i=1ν\{U_{i}\}_{i=1}^{\nu}, and then replace every UiU_{i} with an annulus ViV_{i} which only intersects UiU_{i}. This proves Item a.

b Let f:𝒞𝒢±(S)/N𝒞𝒢±(S)/Nf:\,\mathcal{MCG}^{\pm}(S)/N\to\mathcal{MCG}^{\pm}(S)/N be a (L,L)(L,L)-quasi-isometry which lies within finite distance from the identity. By Item a we know that ff lies within distance RR from the left multiplication by some g¯\overline{g}, which depends only on the induced map f𝒞S/Nf_{\mathcal{C}S/N}. In turn f𝒞S/Nf_{\mathcal{C}S/N} is induced by fHinf_{Hin}, thus if we show that this map is the identity then g¯\overline{g} can be chosen to be the identity, and the corollary follows. Now, for every good hinge σ\sigma, fHin(σ)f_{Hin}(\sigma) was defined in Remark 3.13 as the unique hinge such that dHaus(hfHin(σ),f(hσ))<d_{Haus}(h_{f_{Hin}(\sigma)},f(h_{\sigma}))<\infty. But then, since dHaus(f(hσ),hσ)<d_{Haus}(f(h_{\sigma}),h_{\sigma})<\infty we must have that fHin(σ)=σf_{Hin}(\sigma)=\sigma, that is, fHinf_{Hin} is the identity. ∎

4. Algebraic rigidity

We end the paper by showing that, whenever 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N satisfies Convention 3.2, then the automorphism group of 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N and its abstract commensurator are both isomorphic to 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N itself, via the action of 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N on itself by conjugation. This is Theorem 3 from the introduction, which is covered by Corollaries 4.9 and 4.10 below. The main result of this Section is the following:

Theorem 4.1.

Let SS be either a surface of complexity at least 33 (excluding the case S=S2,0S=S_{2,0}) or a S0,5S_{0,5}, and let 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N satisfy Convention 3.2. Then any isomorphism ϕ:HH\phi:\,H\to H^{\prime} between finite index subgroups of 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N is the restriction of an inner automorphism.

We first recall some definitions and a theorem from [AMS16].

Definition 4.2.

Two elements hh and gg of a group GG are commensurable, and we write hGgh\stackrel{{\scriptstyle G}}{{\approx}}g, if there exist m,n{0}m,n\in\mathbb{Z}\setminus\{0\}, kGk\in G such that kgmk1=hnkg^{m}k^{-1}=h^{n} (that is, if they have non-trivial conjugate powers).

Definition 4.3.

If a group GG acts by isometries on a hyperbolic space 𝒮\mathcal{S}, an element gGg\in G is loxodromic if for some x𝒮x\in\mathcal{S} the map 𝒮\mathbb{Z}\to\mathcal{S}, ngn(x)n\mapsto g^{n}(x) is a quasi-isometric embedding. In the same setting, an element gGg\in G is weakly properly discontinuous, or WPD, if for every ε>0\varepsilon>0 and any x𝒮x\in\mathcal{S} there exists N0=N0(ε,x)N_{0}=N_{0}(\varepsilon,x) such that whenever NN0N\geq N_{0} we have

|{hG|max{dS(x,h(x)),dS(gN(x),hgN(x))}ε}|<\left|\left\{h\in G|\max\left\{d_{S}\left(x,h(x)\right),d_{S}\left(g^{N}(x),hg^{N}(x)\right)\right\}\leq\varepsilon\right\}\right|<\infty

We denote by WPD\mathcal{L}_{WPD} the set of loxodromic WPD elements.

The following result is a special case of [AMS16, Theorem 7.1]. Roughly speaking, the theorem says that if HH is a subgroup of GG and both act “interestingly enough” on some hyperbolic space, then any homomorphism ϕ:HG\phi:H\to G is either (the restriction of) an inner automorphism or it maps some loxodromic WPD to an element which is not commensurable to it.

Theorem 4.4.

Let GG be a group acting coboundedly and by isometries on a hyperbolic space 𝒮\mathcal{S}, with loxodromic WPD elements. Let HGH\leq G be a non-virtually-cyclic subgroup such that HWPDH\cap\mathcal{L}_{WPD}\neq\emptyset, and let EG(H)E_{G}(H) be the unique maximal finite subgroup of GG normalised by HH, whose existence is proven in [AMS16, Lemma 5.6]. Let ϕ:HG\phi:\,H\to G be a homomorphism such that whenever hHWPDh\in H\cap\mathcal{L}_{WPD} then ϕ(h)Gh\phi(h)\stackrel{{\scriptstyle G}}{{\approx}}h. If EG(H)={1}E_{G}(H)=\{1\} then ϕ\phi is the restriction of an inner automorphism.

Our proof of Theorem 4.1 will be very similar to that of [MS23, Theorem 10.1], from which we now abstract a general statement, both for clarity and for later purpose. Recall that a finitely generated group is acylindrically hyperbolic if it is not virtually-cyclic and it acts coboundedly and by isometries on a hyperbolic space 𝒮\mathcal{S}, with loxodromic WPD elements.

Theorem 4.5 (Algebraic rigidity from quasi-isometric rigidity).

Let GG be an acylindrically hyperbolic group. Suppose that GG has no non-trivial finite normal subgroups, and that every self-quasi-isometry of GG is within bounded distance from the left multiplication by some element of GG. Then any isomorphism between finite index subgroups of GG is the restriction of an inner automorphism.

Proof.

We just need to verify that the hypotheses of Theorem 4.4 are satisfied for any isomorphism ϕ:HH\phi:\,H\to H^{\prime} between subgroups of finite index of GG. By definition of acylindrical hyperbolicity, the hypotheses on the action are satisfied. Moreover, GG is not virtually-cyclic, and so also HH is not because its index is finite.

Next, we show that ϕ\phi has the required commensurating property, that is, for every hHWPDh\in H\cap\mathcal{L}_{WPD} we have that ϕ(h)Gh\phi(h)\stackrel{{\scriptstyle G}}{{\approx}}h. Indeed, ϕ\phi can be extended to a quasi-isometry Φ:GG\Phi:\,G\to G (for example, by precomposing ϕ\phi with any closest-point projection GHG\to H). Hence we can find an element gGg\in G whose left-multiplication is uniformly close to Φ\Phi. From here, one can argue as in [MS23, Lemma 10.5], which only uses some basic properties of Cayley graphs of finitely generated groups, to prove that ϕ(h)Gh\phi(h)\stackrel{{\scriptstyle G}}{{\approx}}h whenever hHh\in H has infinite order, and in particular whenever hh is loxodromic WPD.

We are left to prove that EG(H)={1}E_{G}(H)=\{1\}. In view of Lemma [MS23, Lemma 10.6], which holds for any acylindrically hyperbolic group, this follows from the fact that EG(G)={1}E_{G}(G)=\{1\}, i.e. that GG has no non-trivial finite normal subgroups. ∎

Thus to prove Theorem 4.1 we reduced ourselves to verify the hypotheses of Theorem 4.5 when GG is 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N, and SS is as in Theorem 4.1. We know that 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N is quasi-isometrically rigid, by Theorem 3.8, so just need to show that it is acylindrically hyperbolic (Lemma 4.6) and that it has no non-trivial finite normal subgroups (Lemma 4.7). For the first result, we can actually make milder requirements on the topological type of SS:

Lemma 4.6.

Let SS be either a surface of complexity at least 22, and let 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N satisfy Convention 3.2. Then 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N is acylindrically hyperbolic.

Proof.

First of all, 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N is non-virtually-cyclic. Indeed, if x,y𝒞S(0)x,y\in\mathcal{C}S^{(0)} are disjoint curves, then the 2\mathbb{Z}^{2} subgroup generated by the Dehn twists TxT_{x} and TyT_{y} around xx and yy, respectively, intersects NN trivially, since it fixes xx and therefore its minimum displacement is zero. Therefore Tx,Ty\langle T_{x},T_{y}\rangle injects in 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N, which is therefore non-virtually-cyclic.

Now, 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N acts coboundedly on 𝒞S/N\mathcal{C}S/N, because the action is induced by the cobounded action of 𝒞𝒢±(S)\mathcal{MCG}^{\pm}(S) over 𝒞S\mathcal{C}S. Moreover, our Convention 3.2 says that 𝒞S/N\mathcal{C}S/N is hyperbolic and 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N-equivariantly quasi-isometric to the main coordinate space of the HHG structure. Therefore, by [BHS17b, Corollary 14.4] the action admits loxodromic WPD elements provided that 𝒞S/N\mathcal{C}S/N is unbounded, as we noticed in Lemma 3.7. ∎

Lemma 4.7.

Let SS be either a surface of complexity at least 33 (excluding the case S=S2,0S=S_{2,0}) or a S0,5S_{0,5}, and let 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N satisfy Convention 3.2. Then 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N has no non-trivial finite normal subgroup.

Proof.

Let K𝒞𝒢±(S)/NK\leq\mathcal{MCG}^{\pm}(S)/N be a finite normal subgroup, and by contradiction let f¯K\overline{f}\in K be a non-trivial element. If f¯\overline{f} acts trivially on 𝒞S/N\mathcal{C}S/N then f¯\overline{f} is the identity, by the injectivity part of either Theorem 2.1 or Theorem 2.8. Thus let x¯𝒞S/N(0)\overline{x}\in\mathcal{C}S/N^{(0)} be a vertex which is not fixed by f¯\overline{f}. Let x𝒞S(0)x\in\mathcal{C}S^{(0)} be a representative for x¯\overline{x}, let f𝒞𝒢±(S)f\in\mathcal{MCG}^{\pm}(S) be a representative for f¯\overline{f}, let Tx𝒞𝒢±(S)T_{x}\in\mathcal{MCG}^{\pm}(S) be the Dehn Twist around xx, and let Tx¯𝒞𝒢±(S)/N\overline{T_{x}}\in\mathcal{MCG}^{\pm}(S)/N be its image in the quotient. Since KK is finite, we can find m>0m\in\mathbb{N}_{>0} such that f¯=(Tx¯)mf¯(Tx¯)m\overline{f}=(\overline{T_{x}})^{-m}\overline{f}(\overline{T_{x}})^{m}. Hence, denoting by Tf(x)T_{f(x)} the Dehn twist around f(x)f(x), and by 1¯𝒞𝒢±(S)/N\overline{1}\in\mathcal{MCG}^{\pm}(S)/N the identity element of the quotient, we have

1¯=(Tx¯)m(f¯(Tx¯)mf¯1)=(Tx¯)m(Tf(x)¯)m,\overline{1}=(\overline{T_{x}})^{-m}\left(\overline{f}(\overline{T_{x}})^{m}\overline{f}^{-1}\right)=(\overline{T_{x}})^{-m}(\overline{T_{f(x)}})^{m},

where we used how Dehn twists behave under conjugation. In other words, we have that TxmTf(x)mNT_{x}^{-m}T_{f(x)}^{m}\in N.

Now, if x¯\overline{x} and f¯(x¯)\overline{f}(\overline{x}) are adjacent in 𝒞S/N\mathcal{C}S/N, then we could have chosen representatives xx and ff such that xx and f(x)f(x) are disjoint curves. Then TxmTf(x)mT_{x}^{-m}T_{f(x)}^{m} cannot be an element of NN, since it does not have positive displacement.

Hence suppose that x¯\overline{x} and f¯(x¯)\overline{f}(\overline{x}) are not adjacent in 𝒞S/N\mathcal{C}S/N. Let U𝔖U\in\mathfrak{S} be the annulus with core curve xx, let U¯𝔖¯\overline{U}\in\overline{\mathfrak{S}} be its NN-orbit and let ρU¯:𝒞S/N𝒞U¯\rho_{\overline{U}}:\,\mathcal{C}S/N\to\mathcal{C}\overline{U} be the projection given by the HHG structure. Notice that Tx¯\overline{T_{x}} acts on 𝒞U¯\mathcal{C}\overline{U}, since TxT_{x} fixes xx.

Now, (Tx¯)m(Tf(x)¯)m=1¯(\overline{T_{x}})^{-m}(\overline{T_{f(x)}})^{m}=\overline{1}, so it must act as the identity on 𝒞S/N\mathcal{C}S/N, and in particular it must fix f¯(x¯)\overline{f}(\overline{x}). Hence, when we project to 𝒞U¯\mathcal{C}\overline{U} we get

ρ𝒞U¯(f¯(x¯))=ρ𝒞U¯((Tx¯)m(Tf(x)¯)mf¯(x¯))=ρ𝒞U¯((Tx¯)m(f¯(x¯)),\rho_{\mathcal{C}\overline{U}}\left(\overline{f}(\overline{x})\right)=\rho_{\mathcal{C}\overline{U}}\left((\overline{T_{x}})^{-m}(\overline{T_{f(x)}})^{m}\overline{f}(\overline{x})\right)=\rho_{\mathcal{C}\overline{U}}\left((\overline{T_{x}})^{-m}(\overline{f}(\overline{x})\right),

where we used that Tf(x)T_{f(x)} fixes f(x)f(x). Moreover

ρ𝒞U¯((Tx¯)m(f¯(x¯))=(Tx¯)mρ𝒞((Tx¯)m(U¯))(f¯(x¯))=(Tx¯)mρ𝒞U¯(f¯(x¯)),\rho_{\mathcal{C}\overline{U}}\left((\overline{T_{x}})^{-m}(\overline{f}(\overline{x})\right)=(\overline{T_{x}})^{-m}\rho_{\mathcal{C}\left((\overline{T_{x}})^{-m}(\overline{U})\right)}\left(\overline{f}(\overline{x})\right)=(\overline{T_{x}})^{-m}\rho_{\mathcal{C}\overline{U}}\left(\overline{f}(\overline{x})\right),

where we used that projections in a HHG are equivariant with respect to the action of the group. Hence, the action of (Tx¯)m(\overline{T_{x}})^{-m} on 𝒞U¯\mathcal{C}\overline{U} must fix the element ρ𝒞U¯(f¯(x¯))\rho_{\mathcal{C}\overline{U}}\left(\overline{f}(\overline{x})\right).

However, the action of Tx¯\overline{T_{x}} on 𝒞U¯\mathcal{C}\overline{U} was defined via the action of TxT_{x} on 𝒞U\mathcal{C}U, so that the following diagram commutes:

𝒞U{\mathcal{C}U}𝒞U{\mathcal{C}U}𝒞U¯{\mathcal{C}\overline{U}}𝒞U¯{\mathcal{C}\overline{U}}Tx\scriptstyle{T_{x}}\scriptstyle{\cong}\scriptstyle{\cong}Tx¯\scriptstyle{\overline{T_{x}}}

Here the vertical arrows are the restriction to 𝒞U\mathcal{C}U of the quotient projection

UU¯𝒞U𝒞U¯=(UU¯𝒞U)/N.\bigcup_{U^{\prime}\in\overline{U}}\mathcal{C}U^{\prime}\to\mathcal{C}\overline{U}=\left(\bigcup_{U^{\prime}\in\overline{U}}\mathcal{C}U^{\prime}\right)/N.

Such restriction is a quasi-isometry by Convention 3.2. Hence, no power of Tx¯\overline{T_{x}} can fix a point in 𝒞U¯\mathcal{C}\overline{U}, since the action of the Dehn twist TxT_{x} on its annular curve graph 𝒞U\mathcal{C}U is loxodromic. ∎

As a by-product of Theorem 4.1, we get that any automorphism of 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N is the conjugation by some element g¯𝒞𝒢±(S)/N\overline{g}\in\mathcal{MCG}^{\pm}(S)/N. The following lemma states that such g¯\overline{g} is also unique:

Lemma 4.8.

Let SS be either a surface of complexity at least 33 (excluding the case S=S2,0S=S_{2,0}) or S=S0,5S=S_{0,5}, and let 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N satisfy Convention 3.2. Then 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N is centerless.

Proof.

By either Theorem 2.1 or Theorem 2.8, it is enough to show that g¯\overline{g} acts as the identity on 𝒞S/N\mathcal{C}S/N. Notice that g¯\overline{g} commutes with the image of the Dehn twist Tx¯\overline{T_{x}} for any curve x𝒞S(0)x\in\mathcal{C}S^{(0)}. In particular, by how Dehn twists behave under conjugation, we have that Tx¯=Tg(x)¯\overline{T_{x}}=\overline{T_{g(x)}}, where g𝒞𝒢±(S)g\in\mathcal{MCG}^{\pm}(S) is any representative for g¯\overline{g}. Now one can argue as in the proof of Theorem 4.1 to get that g¯(x¯)=x¯\overline{g}(\overline{x})=\overline{x}, and the conclusion follows. ∎

Combining Theorem 4.1 and Lemma 4.8 we get:

Corollary 4.9.

Let SS be either a surface of complexity at least 33 (excluding the case S=S2,0S=S_{2,0}) or S=S0,5S=S_{0,5}, and let 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N satisfy Convention 3.2. Then the map 𝒞𝒢±(S)/NAut(𝒞𝒢±(S)/N)\mathcal{MCG}^{\pm}(S)/N\to\text{Aut}(\mathcal{MCG}^{\pm}(S)/N), which maps an element g¯𝒞𝒢±(S)/N\overline{g}\in\mathcal{MCG}^{\pm}(S)/N to the conjugation by g¯\overline{g}, is an isomorphism. Therefore Out(𝒞𝒢±(S)/N)\text{Out}(\mathcal{MCG}^{\pm}(S)/N) is trivial.

Finally, we recall the definition of the abstract commensurator of a group GG. Consider the set of all isomorphisms HHH\to H^{\prime} between finite-index subgroups of GG. Let Comm(G)\text{Comm}(G) be the quotient of this set by the following equivalence relation: two isomorphisms are identified if they coincide on a finite index subgroup of GG. Then Comm(G)\text{Comm}(G) can be endowed with a group structure, induced by the composition. Our final result shows that Comm(𝒞𝒢±(S)/N)\text{Comm}(\mathcal{MCG}^{\pm}(S)/N) is “the smallest possible”:

Corollary 4.10.

Let SS be either a surface of complexity at least 33 (excluding the case S=S2,0S=S_{2,0}, or S=S0,5S=S_{0,5} and let 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N satisfy Convention 3.2. Then the map 𝒞𝒢±(S)/NComm(𝒞𝒢±(S)/N)\mathcal{MCG}^{\pm}(S)/N\to\text{Comm}(\mathcal{MCG}^{\pm}(S)/N), which maps an element g¯\overline{g} to the conjugation by g¯\overline{g}, is an isomorphism.

Proof.

The map is surjective by Theorem 4.1. Moreover, if the conjugation by g¯\overline{g} coincides with the identity on a finite-index subgroup HH, then g¯\overline{g} commutes with the mm-th power of the image of any Dehn twist, where mm only depends on the index of HH in 𝒞𝒢±(S)/N\mathcal{MCG}^{\pm}(S)/N. Then one can argue as in the proof of Lemma 4.8 to get that g¯\overline{g} acts as the identity on 𝒞S/N\mathcal{C}S/N, and therefore g¯=1¯\overline{g}=\overline{1} by either Theorem 2.1 or Theorem 2.8. ∎

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