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(Non-)Recognizing Spaces for Stable Subgroups

Sahana Balasubramanya, Marissa Chesser, Alice Kerr,
Johanna Mangahas, Marie Trin
Abstract

In this note, we consider the notion of what we call recognizing spaces for stable subgroups of a given group. When a group GG is a mapping class group or right-angled Artin group, it is known that a subgroup is stable exactly when the largest acylindrical action GXG\curvearrowright X provides a quasi-isometric embedding of the subgroup into XX via the orbit map. In this sense the largest acylindrical action for mapping class groups and right-angled Artin groups provides a recognizing space for all stable subgroups. In contrast, we construct an acylindrically hyperbolic group (relatively hyperbolic, in fact) whose largest acylindrical action does not recognize all stable subgroups.

1 Introduction

The quasiconvex subgroups of a hyperbolic group are geometrically natural in that they are exactly the finitely generated quasi-isometrically embedded subgroups (meaning, their geometry reflects that of the ambient group), and consequently they are hyperbolic in their own right [Gro87]. These ideas from Gromov have been widely studied in geometric group theory, and the notion of quasiconvexity now has multiple generalizations to broader settings; see, for example, [FM02, DT15, Gen19, Tra19, AM23].

In this note we are interested in the generalization to stable subgroups of acylindrically hyperbolic groups, specifically those groups admitting a largest acylindrical action; exact definitions of these terms appear in Sections 2.4, 2.1, and 2.3 respectively. Informally, a subgroup HH of a finitely generated group GG is stable when HH is quasi-isometrically embedded in GG and furthermore, quasi-geodesics from GG with common endpoints in HH uniformly fellow-travel. It follows from their definition that stable subgroups are hyperbolic, while the ambient GG typically is not. Acylindrical hyperbolicity vastly generalizes hyperbolicity for groups, as the property requires only some suitable action of GG on some hyperbolic space XX. The set of all such actions for a given group form a partially ordered set, which in certain cases admits a largest element.

Durham and Taylor introduced the notion of stability for both subgroups and subsets of metric spaces [DT15]. Applying a theorem of Aougab–Durham–Taylor [ADT17, Theorem 1.1] to “pull back” stability from metric space to subgroup, we have a sufficient condition for stability of H<GH<G: when GG acts properly on some proper hyperbolic space XX such that the orbit map quasi-isometrically embeds HH in XX. We are interested in the not-quite converse that is the existence of a recognizing space for a stable subgroup of a finitely generated group GG, which we define below. This can be compared to a Morse detectable space, as defined in [RST22].

Definition 1.1.

Let XX be a hyperbolic space equipped with a GG–action. If HH is a stable subgroup of GG, we say XX is a recognizing space for HH if the orbit map quasi-isometrically embeds HH into XX. We call XX a universal recognizing space for GG if it is a recognizing space for all the stable subgroups of GG.

This is not a genuine converse because we lack properness in our motivating examples. Mapping class groups, right angled Artin groups (RAAGs), and, more generally, hierarchically hyperbolic groups (HHGs) each have a well-understood universal recognizing space. Respectively, these are the curve complex [Ham05, pg. 3] [KL08, Theorem 1.3], extension graph [KMT17, Theorem 1.1] and the top level domain of the hierarchy structure [ABD21, Theorem B]. It has recently been shown that CAT(0) groups also have a universal recognizing space, via the curtain model [PSZ22].

In addition to being HHGs, most mapping class groups and RAAGs are also acylindrically hyperbolic groups. In these cases, the recognizing space admits the largest acylindrical action (see subsection 2.1 for details), which does not always exist for an acylindrically hyperbolic group. This prompts the question:

Question 1.2.

If GG is an acylindrically hyperbolic group with a largest acylindrical action on XX, is XX a universal recognizing space for GG?

In other words, does the largest acylindrical action of an acylindrically hyperbolic group, if it exists, contain quasi-isometrically embedded orbits of all of its stable subgroups? We consider this question for the class of (non-elementary) relatively hyperbolic groups, a class of groups introduced by Gromov [Gro87] that generalizes hyperbolic groups. Roughly speaking, the “non-hyperbolic pieces” of such a group are confined to subgroups known as peripheral subgroups, and coning off the cosets of these peripheral subgroups in a Cayley graph for the group yields a hyperbolic space called the relative Cayley graph. In the case that the peripheral subgroups are neither acylindrically hyperbolic nor virtually cyclic, the action on this space is the largest acylindrical action (see subsection 2.3 for details).

Aougab–Durham–Taylor prove equivalence between subgroup stability and quasi-isometric embedding by the orbit map into the relative Cayley graph, in the case where the peripheral subgroups all are one-ended and have linear divergence [ADT17, Theorem 1.5]. Such peripheral groups cannot be acylindrically hyperbolic, as the latter groups contain Morse elements and thus have superlinear divergence [DMS10]. Thus Question 1.2 has a positive answer for a subset of relatively hyperbolic groups, in addition to the HHGs previously mentioned. Furthermore, it was observed by Abbott and Chesser that, if a stable subgroup of a relatively hyperbolic group has finite intersection with each conjugate of every peripheral subgroup, then it quasi-isometrically embeds in the relative Cayley graph via the orbit map.111This follows from [Hru10] Theorem 1.5, Definition 9.6, and Theorem 9.9, along with the fact that stable subgroups are undistorted in the ambient group.. We are then motivated to ask the following refined question.

Question 1.3.

For a relatively hyperbolic group whose peripheral subgroups are neither acylindrically hyperbolic nor virtually cyclic, are there stable subgroups not quasi-isometrically embedded into the relative Cayley graph via the orbit map?

We consider such subgroups not recognized by this action. We provide an affirmative answer to Question 1.3 by constructing a particular relatively hyperbolic group, thereby answering Question 1.2 in the negative. The group we construct is based on a construction of Ol’shanskii, Osin, and Sapir [OOS09, Theorem 1.12]. More precisely, we prove the following.

Theorem 1.4.

There exists a non-elementary relatively hyperbolic (and hence acylindrically hyperbolic) group GG such that

  1. 1.

    GG has a largest acylindrical action on its relative Cayley graph; and

  2. 2.

    GG contains stable subgroups that do not quasi-isometrically embed via the orbit map in the relative Cayley graph.

To the best of our knowledge, this is the first such example to be recorded in the literature. This also prompts some questions for further exploration.

Question 1.5.

Given a relatively hyperbolic group, does it admit a (not necessarily acylindrical) action on some universal recognizing space?

Question 1.6.

If not, does there exist some recognising space for each stable subgroup of a relatively hyperbolic group?

We note here that the examples of groups with universal recognising spaces given previously were either HHGs or CAT(0) groups, and therefore were finitely presented [BHS19, BH99]. In contrast, it follows from [OOS09] that the counterexample we have built is not finitely presented. This raises a further question:

Question 1.7.

For a finitely presented relatively hyperbolic group whose peripheral subgroups are neither acylindrically hyperbolic nor virtually cyclic, is its relative Cayley graph a universal recognising space?

The answers to Questions 1.5 and 1.6 may be hard, as the peripheral subgroups may have no natural action on a hyperbolic space, in contrast with the examples stemming from the HHG case. In particular, Remark 3.1 shows that even if there is a positive answer to Question 1.6, in general it is not possible for all of the actions to be acylindrical. Regarding Question 1.7, to answer it (in the negative) by the same method as for 1.4, we would need to find a finitely presented group which is neither acylindrically hyperbolic nor virtually cyclic, but has an infinite stable subgroup.

Acknowledgements: The authors would like to thank the 2023 Women in Groups, Geometry, and Dynamics program and its organizers for hosting them and providing the opportunity to work together. Our thanks also to Jacob Russell for suggesting helpful references, to Anthony Genevois for the comments contained in Remark 3.3 and to Harry Petyt for raising Question 1.7. The second author thanks Carolyn Abbott for conversations and collaborations that inspired the train of thought that led to this note. Through the fourth author, this work was supported by a grant from the Simons Foundation (965204, JM) and by National Science Foundation Grant No. DMS-1812021. The fifth author is supported by the Centre Henri Lebesgue ANR-11-LABX-0020-01 and the Région Bretagne’s ARED program.

2 Preliminaries

For the sake of keeping our exposition as complete as possible, this section details some background information and results that will be used in the proof of Theorem 1.4. Note that all metric spaces here are assumed to be geodesic.

2.1 Acylindrically hyperbolic groups.

Informally, an acylindrical action can be thought of as a generalization of a proper action, where points are allowed to have large stabilizers, but long cylinders are not. An acylindrically hyperbolic group is a group which acts acylindrically on a hyperbolic space, in a way that is in some sense non-trivial.

Definition 2.1.

An isometric action by a group GG on a metric space (X,d)(X,d) is acylindrical if for every R0R\geqslant 0, there exist N>0N>0 and L>0L>0 such that for every x,yXx,y\in X with d(x,y)Ld(x,y)\geqslant L, we have that

|{gG:d(x,gx)R and d(y,gy)R}|N.|\{g\in G:d(x,gx)\leqslant R\text{ and }d(y,gy)\leqslant R\}|\leqslant N.

An acylindrical action by a group GG on a hyperbolic space XX is non-elementary if GG is not virtually cyclic and orbits are unbounded. A group is acylindrically hyperbolic if it admits a non-elementary acylindrical action on a hyperbolic space.

Over the last few years, the class of acylindrically hyperbolic groups has received considerable attention. It is broad enough to include many examples of interest, e.g., non-elementary hyperbolic and relatively hyperbolic groups (see subsection 2.2), all but finitely many mapping class groups of finite-type surfaces without boundary, non-directly-decomposable RAAGs, outer automorphism groups for free groups of rank at least 2, most 33-manifold groups, and finitely presented groups of deficiency at least 22. On the other hand, the existence of a non-elementary acylindrical action on a hyperbolic space is a rather strong assumption, which allows one to prove non-trivial results. For examples of such results, see [DGO17, Osi16, Osi17], and references therein.

2.2 Relatively hyperbolic groups.

Roughly speaking, a group is relatively hyperbolic group if, when certain subgroups and their conjugates are “coned-off,” the resulting Cayley graph is hyperbolic. This is a more general class than that of hyperbolic groups, which are hyperbolic relative to their trivial subgroup. There are many equivalent definitions of relative hyperbolicity (see for example [Bow12, GM06]). For the purposes of this note, we will use the following as our definition.

Proposition 2.2.

[DGO17, Proposition 4.28] Let GG be a group and {H1,,Hm}\{H_{1},\ldots,H_{m}\} a collection of subgroups of GG. Then GG is hyperbolic relative to {H1,,Hm}\{H_{1},\ldots,H_{m}\} if and only if {H1,,Hm}\{H_{1},\ldots,H_{m}\} is hyperbolically embedded in GG with respect to some finite YGY\subset G.

Being hyperbolically embedded in GG with respect to YY means that YH1HmY\cup H_{1}\cup\cdots\cup H_{m} is a generating set of GG, that Γ(G,YH1Hm)\Gamma(G,Y\sqcup H_{1}\sqcup\cdots\sqcup H_{m}) is hyperbolic, and additionally that this latter Cayley graph satisfies a technical condition we will not use here. We refer to [DGO17, Definition 2.1] for the full description. Note that it also follows from a result of Sisto [Sis16, Theorem 2] that hyperbolically embedded subgroups are quasi-convex, and thus stable when they are hyperbolic.

Definition 2.3.

In the case of Proposition 2.2, {H1,,Hm}\{H_{1},\ldots,H_{m}\} are referred to as peripheral subgroups, and the Cayley graph Γ(G,YH1Hm)\Gamma(G,Y\sqcup H_{1}\sqcup\cdots\sqcup H_{m}) is called the relative Cayley graph.

The following example is well-known (see for example [GM06]) and will be used in the proof of Theorem 1.4. The second statement follows from [Osi06, Corollary 1.5].

Proposition 2.4.

If H1,,HmH_{1},\ldots,H_{m} are groups, then the free product H1HmH_{1}\ast\cdots\ast H_{m} is hyperbolic relative to {H1,,Hm}\{H_{1},\ldots,H_{m}\}. More specifically, H1HmH_{1}\ast\cdots\ast H_{m} is hyperbolic relative to {Hi:Hi is not hyperbolic}\{H_{i}:H_{i}\text{ is not hyperbolic}\}.

Example 2.5.

[DGO17, Example 2.2] Let G=HG=H\ast\mathbb{Z} and =y\mathbb{Z}=\langle y\rangle. Set Y={y}Y=\{y\}. Then HH is hyperbolically embedded in GG with respect to YY. In particular, Γ(G,YH)\Gamma(G,Y\sqcup H) is quasi-isometric to an infinite-diameter tree (see Fig.1), whose “vertices” are copies of the complete Cayley graph ΓH=Γ(H,H)\Gamma_{H}=\Gamma(H,H).

ΓH\Gamma_{H}yΓHy\Gamma_{H}y1ΓHy^{-1}\Gamma_{H}yyy1y^{-1}yyyyy1y^{-1}y1y^{-1}\cdots\cdots\cdots\cdots\cdots\cdots
Figure 1: HH*\mathbb{Z}

Relatively hyperbolic groups fit nicely in between the classes of hyperbolic and acylindrically hyperbolic groups, as shown by the following proposition.

Proposition 2.6.

[Osi16, Proposition 5.2] Let GG be a group that is hyperbolic relative to a collection of subgroups {H1,,Hm}\{H_{1},\ldots,H_{m}\}, and let YGY\subset G be a finite set such that {H1,,Hm}\{H_{1},\ldots,H_{m}\} is hyperbolically embedded in GG with respect to YY. Then GG acts acylindrically on the relative Cayley graph Γ(G,YH1Hm)\Gamma(G,Y\sqcup H_{1}\sqcup\cdots\sqcup H_{m}).

In particular, this means that, so long as Γ(G,YH1Hm)\Gamma(G,Y\sqcup H_{1}\sqcup\cdots\sqcup H_{m}) has infinite diameter and GG is not virtually cyclic, GG is an acylindrically hyperbolic group. Such relatively hyperbolic groups are referred to as non-elementary.

2.3 Largest acylindrical actions

For any group GG, one can study the set of cobounded acylindrical actions of GG on hyperbolic spaces, and ask if this set has a largest action. It follows from [ABO19, Lemma 3.11] that this is equivalent to considering the (possibly infinite) generating sets YY of GG such that the Cayley graph Γ(G,Y)\Gamma(G,Y) is hyperbolic and GΓ(G,Y)G\curvearrowright\Gamma(G,Y) is acylindrical:

Definition 2.7.

Let GG be a group, and YGY\subset G be a generating set. The action GΓ(G,Y)G\curvearrowright\Gamma(G,Y) is the largest acylindrical action if Γ(G,Y)\Gamma(G,Y) is hyperbolic and GΓ(G,Y)G\curvearrowright\Gamma(G,Y) is acylindrical, and if for every other generating set SGS\subset G such that Γ(G,S)\Gamma(G,S) is hyperbolic and GΓ(G,S)G\curvearrowright\Gamma(G,S) is acylindrical, the identity map of GG induces a Lipschitz map Γ(G,Y)Γ(G,S)\Gamma(G,Y)\to\Gamma(G,S).

Questions about largest actions were considered extensively in [ABO19], and we refer the reader to the introduction and initial sections of that note for more precise definitions.

Remark 2.8.

By [ABO19, Theorem 2.6], if a group GG is not acylindrically hyperbolic, then its largest acylindrical action is realised either by taking GG itself to be the generating set, or, in the case that GG is virtually cyclic, by any finite generating set of GG. This means that the existence of a largest acylindrical action is non-trivial only if the group is acylindrically hyperbolic.

Even though there are examples of acylindrically hyperbolic groups that do not admit a largest acylindrical action, (see [ABO19, Example 7.2 and Theorem 7.3]), it turns out that many groups classically studied in geometric group theory do:

Theorem 2.9.

[ABO19, Theorem 2.18] [ABD21, Theorem A] The following groups have largest acylindrical actions:

  1. (a)

    Hyperbolic groups.

  2. (b)

    Finitely generated relatively hyperbolic groups whose peripheral subgroups are not acylindrically hyperbolic.

  3. (c)

    Hierarchically hyperbolic groups, which includes mapping class groups of orientable surfaces of finite type and right-angled Artin groups.

  4. (d)

    Fundamental groups of compact orientable 33-manifolds with empty or toroidal boundary.

In all of these cases, the space on which the group has its largest action is well understood. As mentioned in the introduction, these spaces are universal recognizing spaces for (a) and (c). For the relatively hyperbolic groups in (b), the largest acylindrical action is on the relative Cayley graph:

Theorem 2.10.

[ABO19, Theorem 2.18] Let GG be a finitely generated relatively hyperbolic groups whose peripheral subgroups {H1,,Hm}\{H_{1},\ldots,H_{m}\} are neither acylindrically hyperbolic nor virtually cyclic. Let YGY\subset G be a finite set such that {H1,,Hm}\{H_{1},\ldots,H_{m}\} is hyperbolically embedded in GG with respect to YY. The largest acylindrical action of GG is on the relative Cayley graph Γ(G,YH1Hm)\Gamma(G,Y\sqcup H_{1}\sqcup\cdots\sqcup H_{m}).

2.4 Stable subgroups of relatively hyperbolic groups.

Stable subgroups of an arbitrary finitely generated group are defined as follows.

Definition 2.11.

Let GG be a finitely generated group. A finitely generated subgroup KGK\leq G is said to be stable if these conditions both hold:

  1. 1.

    KK is undistorted in GG, meaning KK quasi-isometrically embeds into GG with respect to their respective finite generating sets.

  2. 2.

    For any constants (λ,C)(\lambda,C), there is a constant M>0M>0 (depending on λ,C\lambda,C) such that any two (λ,C)(\lambda,C)–quasi-geodesics with the same end points in KK are MM–close to each other.

When the ambient group is relatively hyperbolic, stable subgroups can also be characterised in terms of how they intersect conjugates of peripheral subgroups.

Theorem 2.12.

[Tra19, Corollary 1.10] Let GG be a finitely generated relatively hyperbolic groups with peripheral subgroups {H1,,Hm}\{H_{1},\ldots,H_{m}\}. Let KK be a finitely generated undistorted subgroup of GG. Then the following are equivalent:

  1. 1.

    KK is stable in GG

  2. 2.

    For every peripheral subgroup HiH_{i}, KHigK\cap H_{i}^{g} is stable in HigH_{i}^{g} for each conjugate HigH_{i}^{g}

  3. 3.

    For every peripheral subgroup HiH_{i}, KHigK\cap H_{i}^{g} is stable in GG for each conjugate HigH_{i}^{g}

We would like to use this to construct an example of a relatively hyperbolic group with a stable subgroup not recognised by the relative Cayley graph. In this context, one useful property of peripheral subgroups is the following.

Lemma 2.13.

[Bow12] Let GG be hyperbolic relative to {H1,,Hm}\{H_{1},\ldots,H_{m}\}. Then for every g,hGg,h\in G and i,j{1,,m}i,j\in\{1,\ldots,m\}, if the conjugates HigH_{i}^{g} and HjhH_{j}^{h} are not equal, then their intersection is finite.

As any finite subgroup is stable, which can be seen directly from Definition 2.11, we observe the following corollary to Theorem 2.12.

Corollary 2.14.

Let GG be a finitely generated relatively hyperbolic groups with peripheral subgroups {H1,,Hm}\{H_{1},\ldots,H_{m}\}. Let KK be a finitely generated undistorted subgroup of GG. Suppose that KK is a subgroup of some HiH_{i}, and that KK is stable in HiH_{i}. Then KK is stable in GG.

3 Proof of Main Theorem

Proof of Theorem 1.4.

By [OOS09, Theorem 1.12], there exists a finitely generated group HH such that every proper subgroup is infinite cyclic, while HH itself is not virtually cyclic. Moreover, for any finite generating set SS of HH, [OOS09, Theorem 1.12] states that every periodic path in the Cayley graph Γ(H,S)\Gamma(H,S) is a Morse quasi-geodesic. In particular, for every nontrivial qHq\in H, we have that q\langle q\rangle is Morse and hyperbolic, which implies that q\langle q\rangle is stable in HH by [Tra19, Proposition 4.3].

Consider G=HG=H\ast\mathbb{Z}, where yy is the generator of \mathbb{Z}. Then GG is finitely generated by {y}S\{y\}\cup S. Recall from Proposition 2.4 that GG is relatively hyperbolic with peripheral subgroup HH. By Example 2.5 and Proposition 2.6, GG is also acylindrically hyperbolic. However, as the peripheral subgroup HH contains no non-abelian free subgroups, HH is not acylindrically hyperbolic (as such groups have independent loxodromics acting on a hyperbolic space, which allows one to construct a rank-two free group by the standard ping-pong argument; see for example [Gro87, Osi16]). It follows from Theorem 2.9(b) and Theorem 2.10 that GG admits a largest acylindrical action on the relative Cayley graph Γ(G,{y}H)\Gamma(G,\{y\}\sqcup H).

Recall that for every nontrivial qHq\in H, we have that q\langle q\rangle is stable in HH. As GG is a free product, any path with endpoints in Γ(H,S)\Gamma(H,S), which also leaves Γ(H,S)\Gamma(H,S), must visit the same point twice. We therefore have that Γ(H,S)\Gamma(H,S) isometrically embeds into Γ(G,{y}S)\Gamma(G,\{y\}\cup S). As q\langle q\rangle is a quasi-geodesic in HH, we automatically get that q\langle q\rangle is a quasi-geodesic in GG, and so is undistorted in GG. It therefore follows from Corollary 2.14 that q\langle q\rangle is stable in GG. However, q\langle q\rangle is clearly not quasi-isometrically embedded in the relative Cayley graph Γ(G,{y}H)\Gamma(G,\{y\}\sqcup H), as the orbit of HH is bounded therein, and qq has infinite order. ∎

Remark 3.1.

In fact, no acylindrical action of GG on a hyperbolic space can recognize the stable subgroup q\langle q\rangle. Indeed, if GXG\curvearrowright X is an acylindrical action on a hyperbolic space, then it follows that the restriction of the action to HH is also acylindrical. As HH is not acylindrically hyperbolic, and is not virtually cyclic, the action of HH must have bounded orbits. Consequently q\langle q\rangle cannot be quasi-isometrically embedded in XX, as that would imply that HH has an unbounded orbit, which is a contradiction. In other words, any positive answer to Question 1.5 in this case would be via a non-acylindrical action. Regarding Question 1.6, even if recognizing spaces exist for each individual stable subgroup of GG, this means that some of the actions will not be acylindrical.

Remark 3.2.

Note that the stability of q\langle q\rangle in the above proof of Theorem 1.4 can also be seen directly. The fact that q\langle q\rangle is quasi-isometrically embedded in the Cayley graph Γ(G,{y}S)\Gamma(G,\{y\}\cup S) is already addressed directly in the proof; one can also see directly that the uniform fellow-traveling of quasi-geodesics is satisfied. In particular, we may view Γ(G,{y}S)\Gamma(G,\{y\}\cup S) in a manner similar to that in Figure 1, with the complete subgraph Γ(H,H)\Gamma(H,H) replaced with copies of Γ(H,S)\Gamma(H,S). This is still a space with a “tree-like” structure. Suppose σ\sigma is a quasi-geodesic in Γ(G,{y}S)\Gamma(G,\{y\}\cup S) that starts and ends in qΓ(H,S)\langle q\rangle\subset\Gamma(H,S), and let qσ\langle q\rangle_{\sigma} be the segment of q\langle q\rangle with the same endpoints as σ\sigma. The lengths of segments of σ\sigma that leave Γ(H,S)\Gamma(H,S) are bounded uniformly (depending on the quasi-geodesic constants), as they must eventually return to the same point from where they left Γ(H,S)\Gamma(H,S). As the segments of σ\sigma that remain in Γ(H,S)\Gamma(H,S) form a quasi-geodesic, and qσ\langle q\rangle_{\sigma} is itself a quasi-geodesic, by the stability of q\langle q\rangle in HH it follows that σ\sigma stays uniformly close to qσ\langle q\rangle_{\sigma}. The same is true of any other quasi-geodesic with the same constants and endpoints as σ\sigma, and therefore q\langle q\rangle is stable in GG.

Remark 3.3.

We note that the only properties used about the group HH from [OOS09] is that it is finitely generated and contains Morse elements, but is neither acylindrically hyperbolic nor virtually cyclic. As very few such examples are known, it would be interesting to consider if there exist groups containing Morse elements with even worse “un-hyperbolic-like” properties. For instance, does there exist a group AA (resp. finitely presented group AA) with Morse elements with the Property (NL)\mathrm{(NL)} (i.e. admitting no actions on hyperbolic spaces with loxodromic elements; see [BFGS22])? If so, Question 1.6 (resp. Question 1.7) automatically will have a negative answer by considering the free product G=AG=A\ast\mathbb{Z}. As it is unclear if the group from [OOS09] has property (NL)\mathrm{(NL)}, we leave such explorations for future work.

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