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On the Girth of Groups Acting on CAT(0) Cube Complexes

Arka banerjee Auburn University, 221 Parker Hall, Auburn, AL 36849, USA [email protected] Daniel Gulbrandsen Adams State University, 208 Edgemont Blvd, Alamosa, CO 81101, USA [email protected] Pratyush Mishra Wake Forest University, 127 Manchester Hall, Winston-Salem, NC 27109, USA [email protected]  and  Prayagdeep Parija Virginia Tech, Mcbryde Hall, 225 Stranger Street, Blacksburg, VA 24060, USA [email protected]
Abstract.

We obtain a sufficient condition for lattices in the automorphism group of a finite dimensional CAT(0) cube complex to have infinite girth. As a corollary, we get a version of Girth Alternative for groups acting geometrically: any such group is either {locally finite}-by-{virtually abelian} or it has infinite girth. We produce counterexamples to show that the alternative fails in the general class of groups acting cocompactly on finite dimensional CAT(0) cube complexes by obtaining examples of non-virtually solvable groups which satisfy a law.

Key words and phrases:

1. Introduction

The girth of a finite graph is defined as the length of its shortest non-trivial cycle. If the graph has no cycle then its girth is defined to be infinite. Given a finitely generated group Γ\Gamma with a fixed generating set SS, it makes sense to talk about the girth of it’s Cayley graph, denoted Girth(Cay(Γ,S))\operatorname{Girth}(\operatorname{Cay}(\Gamma,S)). Then, one can define the girth of the group Γ\Gamma as the supremum of the girth of the Cayley graphs over all finite generating sets SS of Γ,\Gamma, i.e.

Girth(Γ)=supΓ=S,|S|<{Girth(Cay(Γ,S))}\operatorname{Girth}(\Gamma)=\sup_{\Gamma=\langle S\rangle,|S|<\infty}\bigg{\{}\operatorname{Girth}(\operatorname{Cay}(\Gamma,S))\bigg{\}}

Note that Girth(Cay(Γ,S))\operatorname{Girth}(\operatorname{Cay}(\Gamma,S)) measures the length of the shortest non-trivial word relation in the Cayley graph Cay(Γ,S)\operatorname{Cay}(\Gamma,S). Some examples of groups with finite girth are finite groups, non-cyclic nilpotent groups and solvable groups. In fact, any finitely generated group satisfying a non-trivial law has finite girth, [Sch01], [Akh03]. Moreover, if a group has a finite index subgroup with finite girth, then the group itself has finite girth [see [Sch01] for details]. In particular, virtually solvable groups have finite girth. On the other hand, any free group has infinite girth, in particular \mathbb{Z} has infinite girth (which can be seen as a degeneracy case).

Given a class of groups, it is natural to ask if one can classify each group in the class in terms of finite and infinite girth. Motivated by the celebrated Tits Alternative [Tit72], Girth Alternative [Akh05] is defined as follows.

Girth Alternative: For a given class 𝒞\mathcal{C} of finitely generated groups, 𝒞\mathcal{C} is said to satisfy the Girth Alternative if for any group Γ𝒞\Gamma\in\mathcal{C}, either Γ\Gamma is virtually solvable (and hence has finite girth unless isomorphic to \mathbb{Z}) or girth of Γ\Gamma is infinite.

The Girth Alternative is similar in spirit to the Tits Alternative (which was first introduced by Jacques Tits in 1972, where he proved the alternative for the class of linear groups). For a general class of groups, the Tits Alternative can be stated as follows.

Tits Alternative: For a given class 𝒞\mathcal{C} of finitely generated groups, 𝒞\mathcal{C} is said to satisfy Tits Alternative if for any group Γ𝒞\Gamma\in\mathcal{C}, either Γ\Gamma is virtually solvable or Γ\Gamma contains a non-abelian free subgroup 𝔽2\mathbb{F}_{2}.

Some classes of finitely generated groups satisfying the Tits Alternative are linear groups ([Tit72]), Gromov hyperbolic groups (follows from the fact that it contains a cyclic subgroup of finite index or 𝔽2\mathbb{F}_{2} as a subgroup, see Theorem 5.3.E in [Gro87]), mapping class groups of compact surfaces ([Iva84], [BLM83]), Out(𝔽n\mathbb{F}_{n}) ([BFH97], [BFH97a]), groups acting on CAT(0) cube complex ([SW05], [CS11]), etc. On the other hand, Thompson’s group F does not satisfy Tits Alternative: neither Thompson’s group F contains a copy of 𝔽2\mathbb{F}_{2} ([BS85]) nor it is virtually solvable ([Ble05]).

It has been observed that for certain classes of groups for which Tits Alternative holds, the property of having infinite girth coincides with the property of containing a non-abelian free group 111Although, this observation does not seem to hold in general, see [Akh24]. A comprehensive theory of the Girth Alternative for different classes of groups has been developed by many authors in the past two decades. In [Akh03], [Akh05], Akhmedov has introduced and proved the Girth Alternative for the class of hyperbolic, linear, one-relator and PL+(I)\mbox{PL}_{+}(I) groups. In [Yam11], Yamagata proves the Girth Alternative for convergence groups and irreducible subgroups of the mapping class groups. Independently in [Nak14], Nakamura proves the Alternative for all subgroups of mapping class groups and also for the subgroups of Out(𝔽n\mathbb{F}_{n}) containing the irreducible elements having irreducible powers. Recently, Akhmedov and the third author of this article have studied the Girth Alternative phenomenon for HNN extensions and amalgamated free products [AM23].

Therefore, it is natural to study the Girth Alternative for the class of groups for which Tits Alternative has been investigated. In this paper, we focus on groups acting on CAT(0)\operatorname{CAT(0)} cube complex. Different versions of Tits Alternative for groups acting on CAT(0) cube complex are known from the work of Sageev–Wise [SW05] and Caprace–Sageev [CS11]. Inspired by the work of Caprace–Sageev [CS11], we prove a Girth Alternative for lattices in the group of automorphisms of finite dimensional cube complex.

Theorem A.

Let X=X1××XnX=X_{1}\times\dots\times X_{n} be a product of nn irreducible, unbounded, and locally compact CAT(0)\operatorname{CAT(0)} cube complexes such that Aut(Xi)\mathop{\mathrm{Aut}}\nolimits(X_{i}) acts cocompactly and essentially on XiX_{i} for all ii.

Then for any (possibly non-uniform) lattice ΓAut(X)\Gamma\leq\mathop{\mathrm{Aut}}\nolimits(X) acting properly on XX, either Γ\Gamma is {locally finite}-by-{virtually abelian} or Girth(Γ)=\operatorname{Girth}(\Gamma)=\infty.

Note that if a group has an upper bound on the order of the finite subgroups then any locally finite subgroup of that group has finite order. Therefore, the following is an immediate consequence of Theorem A.

Corollary B.

Let X=X1××XnX=X_{1}\times\dots\times X_{n} be a product of nn irreducible, unbounded, and locally compact CAT(0)\operatorname{CAT(0)} cube complexes such that Aut(Xi)\mathop{\mathrm{Aut}}\nolimits(X_{i}) acts cocompactly and essentially on XiX_{i} for all ii. Suppose ΓAut(X)\Gamma\leq\mathop{\mathrm{Aut}}\nolimits(X) is a lattice (possibly non-uniform) acting properly on XX and Γ\Gamma has a bound on the order of its finite subgroups.

Then Γ\Gamma is either virtually abelian or Girth(Γ)=\operatorname{Girth}(\Gamma)=\infty. In particular, Γ\Gamma satisfies the Girth Alternative.

We obtain Theorem A as a consequence of the (proof of) following more general theorem that gives sufficient conditions for a lattice to have infinite girth.

Theorem C.

Let X=X1××XnX=X_{1}\times\dots\times X_{n} be a product of nn irreducible, unbounded, locally compact CAT(0)\operatorname{CAT(0)} cube complexes such that Aut(Xi)\mathop{\mathrm{Aut}}\nolimits(X_{i}) acts cocompactly and essentially on XiX_{i} for all ii.

Then for any (possibly non-uniform) lattice ΓAut(X)\Gamma\leq\mathop{\mathrm{Aut}}\nolimits(X), either Γ\Gamma virtually fixes some point in XXX\cup\partial_{\infty}X or Girth(Γ)=\operatorname{Girth}(\Gamma)=\infty.

In contrast to the above theorems, it is also interesting to investigate groups which do not satisfy Girth Alternative. This essentially boils down to finding groups satisfying a law, but which are not virtually solvable. In [CM07], the authors produce such examples of groups. More precisely, they construct finitely generated residually p-groups which satisfy a law, but are not virtually solvable. In fact, their examples show that both the Girth Alternative and Tits Alternative fail for the class of residually finite groups. However, we do not know if the examples of Cornulier and Mann can be realized as groups acting on CAT(0) cube complex. Therefore, we provide our own counterexample in Section 4 to show that Girth Alternative, as stated in Corollary B, fails for the class of groups acting cocompactly on finite dimensional CAT(0) cube complexes.

Sketch of proof for Theorem C.

There are three main ingredients used in our proof. The first is a theorem of Nakamura [Nak14] (see Theorem 4) that gives a sufficient condition for a group to have infinite girth. In particular, the condition asks for two elements that generate a free subgroup. In order to ensure such elements always exist under the hypotheses of Theorem C, we use our second ingredient, which is a theorem of Caprace and Sageev [CS11] (see Theorem 5). However, infinite girth does not follow just from a non-abelian free subgroup. Rather, it follows from more subtle properties of generators of the free subgroup, which are required by Nakamura’s theorem. To account for these extra properties, we have to choose ‘correct’ generators. To this end we use our third ingredient, Lemma 6, which asserts the existence of lots of mutually disjoint halfspaces in the cube complex under certain conditions. Combining ingredients two and three yields infinitely many candidates for generators of different free subgroups. The primary objective in the proof of Theorem C is then to find the ‘correct’ generators from this lot that satisfy the properties needed to apply Nakamura’s theorem. As a result, we obtain infinite girth.

Overview.

The paper is organized as follows. In Section 2, we discuss some basic concepts pertaining to the theory of CAT(0) cube complexes. Readers who are familiar with CAT(0) cube complexes may skip this section. We prove Theorem C and Theorem A in Section 3 where they appear as Theorem 10 and Theorem 11, respectively. In Section 4, we give an example which shows Corollary B does not hold if both the assumptions properness and having a bound on the order of finite subgroups are omitted.

2. Preliminaries

2.1. Cube Complexes

Let I=[0,1]I=[0,1]. We define an nn-cube, or simply cube, as the product InI^{n} (with I0={0}I^{0}=\{0\}). A face of InI^{n} is the restriction of some number (possibly zero) of its coordinates to 0 or 11, and a midcube of InI^{n} is the restriction of precisely one of its coordinates to 1/21/2. Cleary, midcubes of InI^{n} can be realized as (n1)(n-1)-cubes and we will often treat them as such. We will refer to 0-cubes, 11-cubes, and 22-cubes as vertices, edges, and squares respectively.

A cube complex is a cell complex where the cells are nn-cubes, for various nn, and the attaching maps are Euclidean isometries in faces. We say the dimension of a cube complex XX is nn, or XX is finite dimensional, if XX contains nn-cubes but not (n+1)(n+1)-cubes, for some nn. If no such nn exists, we say that XX is infinite dimensional. XX is locally finite if every vertex of XX meets only finitely many cubes. In the setting of cube complexes, being locally finite is equivalent to being locally compact.

Two cube complexes XX and YY are isomorphic if there is a bijection ϕ\phi between their vertex sets such that, if cc is an nn-cube in XX then ϕ(c)\phi(c) is an nn-cube in YY. In particular, an isomorphism of cube complexes maps adjacent vertices to adjacent vertices.

A subcomplex YY of a cube complex XX is any collection of cubes in XX inheriting the same attaching maps. We will denote subcomplexes by YXY\leq X. We call XX irreducible if there do not exist cube complexes X1,X2X_{1},X_{2} with X=X1×X2X=X_{1}\times X_{2}. Note that, if X=X1×X2X=X_{1}\times X_{2}, then XX contains subcomplexes isomorphic to X1X_{1} and X2X_{2}. Cube complexes need not be connected.

A cube complex XX is a CAT(0) space if extending the Euclidean metric on individual cubes to the path length metric on XX yields a CAT(0) space, in the traditional sense. That is, triangles are at least as thin as their comparison triangles in Euclidean space. Due to Gromov [Gro87], there is a combinatorial requirement that, if satisfied by XX, will guarantee that XX is locally CAT(0). A finite dimensional cube complex XX is locally CAT(0) if the link of every vertex in XX is a simplicial flag complex. If, in addition, XX is simply-connected then being locally CAT(0) implies that XX is CAT(0). The equivalence between the being locally CAT(0) and (locally) satisfying the classical definition of CAT(0) was extended to infinite dimensional CAT(0) cube complexes in [Lea13].

From now on, unless stated otherwise, all cube complexes considered are assumed to be CAT(0), locally finite, and finite dimensional. Note that for all such cube complexes XX, the decomposition X=X1××XnX=X_{1}\times\cdots\times X_{n} into irreducible factors is unique up to a permutation of its factors by the following proposition.

Proposition 1 ([CS11]).

A finite dimensional CAT(0)\operatorname{CAT(0)} cube complex XX admits a canonical decomposition

X=X1×X2××XpX=X_{1}\times X_{2}\times\ldots\times X_{p}

into a product of irreducible cube complexes XiX_{i}. Every automorphism of XX preserves that decomposition, up to a permutation of possibly isomorphic factors. In particular, the image of canonical embedding

Aut(X1)×Aut(X2)××Aut(Xp)Aut(X)\mathop{\mathrm{Aut}}\nolimits(X_{1})\times\mathop{\mathrm{Aut}}\nolimits(X_{2})\times\ldots\times\mathop{\mathrm{Aut}}\nolimits(X_{p})\hookrightarrow\mathop{\mathrm{Aut}}\nolimits(X)

has finite index in Aut(X)\mathop{\mathrm{Aut}}\nolimits(X).

When it is necessary to treat XX as a metric space, we will use dd to denote the CAT(0) metric. With this metric, XX is a unique geodesic space.

2.2. Hyperplanes and Halfspaces

For a cube complex XX, we say two edges e1,e2Xe_{1},e_{2}\in X are related if e1e2=e_{1}\cap e_{2}=\emptyset and there is a square in XX containing e1e_{1} and e2e_{2}.

Informally, e1e_{1} and e2e_{2} are related if they are opposite edges of a square. A hyperplane in XX, typically denoted as 𝔥^\hat{\mathfrak{h}}, is the transitive closure of this relation on a single edge. The collection of all hyperplanes in a cube complex XX is denoted ^X\hat{\mathcal{H}}_{X}. For the geometric realization of a hyperplane, first observe that any nonempty collection of related edges in an nn-cube cc uniquely determine a midcube of cc. Midcubes in XX therefore inherit a relation from the edges. One then sees that two midcubes MM and NN are related whenever their intersection is a common face. The geometric realization of 𝔥^\hat{\mathfrak{h}} is the transitive closure of this relation on a single midcube. In this instance, midcubes MM and NN inherit attaching maps from their corresponding cubes.

For the remainder, we use the same symbol, 𝔥^\hat{\mathfrak{h}}, to denote both a hyperplane and its geometric realization.

Two hyperplanes 𝔥^1\hat{\mathfrak{h}}_{1} and 𝔥^2\hat{\mathfrak{h}}_{2} are transverse, denoted 𝔥^1𝔥^2\hat{\mathfrak{h}}_{1}\pitchfork\hat{\mathfrak{h}}_{2}, if there is a square in XX containing edges e1e_{1} and e2e_{2} with e1𝔥^1,e2𝔥^2e_{1}\in\hat{\mathfrak{h}}_{1},\;e_{2}\in\hat{\mathfrak{h}}_{2}, and e1e2e_{1}\cap e_{2}\neq\emptyset. Note that 𝔥^1𝔥^2\hat{\mathfrak{h}}_{1}\pitchfork\hat{\mathfrak{h}}_{2} if and only if their geometric realizations intersect. If 𝔥^1\hat{\mathfrak{h}}_{1} and 𝔥^2\hat{\mathfrak{h}}_{2} are not transverse, they are nested. We say 𝔥^1\hat{\mathfrak{h}}_{1} and 𝔥^2\hat{\mathfrak{h}}_{2} are separated if there is a third hyperplane containing 𝔥^1\hat{\mathfrak{h}}_{1} and 𝔥^2\hat{\mathfrak{h}}_{2} in complimentary halfspaces, and they are strongly separated if they are separated and there does not exist a hyperplane transverse to both 𝔥^1\hat{\mathfrak{h}}_{1} and 𝔥^2\hat{\mathfrak{h}}_{2}.

Properties of Hyperplanes. Let XX be a CAT(0) cube complex and 𝔥^^X\hat{\mathfrak{h}}\in\hat{\mathcal{H}}_{X}

  1. (1)

    𝔥^\hat{\mathfrak{h}} is a CAT(0) cube complex in its own right.

  2. (2)

    𝔥^\hat{\mathfrak{h}} separates XX into two components.

Recent proofs of these properties can be found in [Far16]. We denote the closures of the two components of X𝔥^X\setminus\hat{\mathfrak{h}} by 𝔥{\mathfrak{h}} and 𝔥{\mathfrak{h}}^{*}, which we also refer to as halfspaces. Choosing which component to call 𝔥{\mathfrak{h}} for all 𝔥^^X\hat{\mathfrak{h}}\in\hat{\mathcal{H}}_{X} defines a labeling of ^X\hat{\mathcal{H}}_{X}. The collection of halfspaces of XX is denoted X\mathcal{H}_{X}. A halfspace 𝔥{\mathfrak{h}} is deep if the distance from 𝔥^\hat{\mathfrak{h}} to points in 𝔥{\mathfrak{h}} is unbounded. Otherwise, 𝔥{\mathfrak{h}} is shallow. Halfspaces 𝔥1{\mathfrak{h}}_{1} and 𝔥2{\mathfrak{h}}_{2} are nested if either 𝔥1𝔥2{\mathfrak{h}}_{1}\subset{\mathfrak{h}}_{2} or 𝔥2𝔥1{\mathfrak{h}}_{2}\subset{\mathfrak{h}}_{1}. Note that if hyperplanes 𝔥^1\hat{\mathfrak{h}}_{1} and 𝔥^2\hat{\mathfrak{h}}_{2} are nested then they each have a halfspace which together form a nested pair. We also call 𝔥1{\mathfrak{h}}_{1} and 𝔥2{\mathfrak{h}}_{2} strongly separated if 𝔥^1\hat{\mathfrak{h}}_{1} and 𝔥^2\hat{\mathfrak{h}}_{2} are strongly separated.

2.3. Boundaries and Regular Points

The collection of halfspaces of a CAT(0) cube complex XX forms a poset with partial order given by set-inclusion, and comes naturally equipped a complimentary map given by the involution 𝔥𝔥{\mathfrak{h}}\to{\mathfrak{h}}^{*}. Let X\mathcal{H}_{X}^{\circ} denote the collection of ultrafilters of X\mathcal{H}_{X}, that is, αX\alpha\in\mathcal{H}_{X}^{\circ} satisfies the two conditions

  1. (1)

    (Choice) for every pair 𝔥,𝔥X{\mathfrak{h}},{\mathfrak{h}}^{*}\in\mathcal{H}_{X}, exactly one of them is in α\alpha, and

  2. (2)

    (Consistency) if 𝔥1α{\mathfrak{h}}_{1}\in\alpha and 𝔥2X{\mathfrak{h}}_{2}\in\mathcal{H}_{X} with 𝔥1𝔥2{\mathfrak{h}}_{1}\subset{\mathfrak{h}}_{2}, then 𝔥2α{\mathfrak{h}}_{2}\in\alpha.

Given an ultrafilter αX\alpha\in\mathcal{H}_{X}^{\circ}, any subset {𝔥i}α\{{\mathfrak{h}}_{i}\}\subseteq\alpha is guaranteed to satisfy the so called partial choice condition: for every pair 𝔥,𝔥{\mathfrak{h}},{\mathfrak{h}}^{*}, at most one of them is in α\alpha.

A nested sequence of halfspaces {𝔥i}\{{\mathfrak{h}}_{i}\} is called descending (or a descending chain) if 𝔥i+1𝔥i{\mathfrak{h}}_{i+1}\subseteq{\mathfrak{h}}_{i} for all ii. A descending sequence of halfspaces is terminating if 𝔥j=𝔥N{\mathfrak{h}}_{j}={\mathfrak{h}}_{N}, for some NN and all j>Nj>N. Otherwise {𝔥i}\{{\mathfrak{h}}_{i}\} is nonterminating. Given σX\sigma\in\mathcal{H}_{X}^{\circ}, we say σ\sigma satisfies the descending chain condition (DCC) if every descending sequence in σ\sigma is terminating. Note that descending sequences necessarily satisfy the partial choice condition.

One has a bijective correspondence between the vertex set of XX and ultrafilters in X\mathcal{H}_{X}^{\circ} satisfying the DCC given by θ:X0\theta:X^{0}\to\mathcal{H}^{\circ}, where θ(v)={𝔥X|v𝔥}\theta(v)=\{{\mathfrak{h}}\in\mathcal{H}_{X}\;|\;v\in{\mathfrak{h}}\}. Given a vertex vXv\in X, choosing the halfspace containing vv to call 𝔥{\mathfrak{h}} for all hyperplanes 𝔥^\hat{\mathfrak{h}} gives a labeling of ^X\hat{\mathcal{H}}_{X}, which we refer to as being determined by vv.

Now, let 𝟐:={𝟎,𝟏}\bf{2}:=\{0,1\}. Then 𝟐^\bf{2}^{\hat{\mathcal{H}}} is compact in the Tychonoff topology and the choice condition induces an inclusion X𝟐^\mathcal{H}_{X}^{\circ}\hookrightarrow{\bf 2}^{\hat{\mathcal{H}}} in which X\mathcal{H}_{X}^{\circ} embeds as a closed subset which is therefore compact. We call the image of X\mathcal{H}_{X}^{\circ} the Roller compactification and denote it by X¯\bar{X}. To realize the image of X0X^{0} in 𝟐^\bf{2}^{\hat{\mathcal{H}}} concretely, start by defining ϕ𝔥^:X0𝟐\phi_{\hat{\mathfrak{h}}}:X^{0}\to\bf{2} by

ϕ𝔥^(v)={1ifx𝔥0ifx𝔥\phi_{\hat{\mathfrak{h}}}(v)=\left\{\begin{array}[]{cc}1&{\rm if}\;x\in{\mathfrak{h}}\\ 0&\;{\rm if}\;x\in{\mathfrak{h}}^{*}\end{array}\right.

Then, the map with coordinate functions {ϕ𝔥^}𝔥^^\{\phi_{\hat{\mathfrak{h}}}\}_{\hat{\mathfrak{h}}\in\hat{\mathcal{H}}} gives an embedding X0X¯X^{0}\hookrightarrow\bar{X} as a dense open subset. See [Rol16] and [NS13] for details. Note that the Roller compactification behaves well with respect to products. Indeed, if X=X1××XnX=X_{1}\times\cdots\times X_{n} then X¯=X¯1××X¯n\bar{X}=\bar{X}_{1}\times\cdots\times\bar{X}_{n}. The Roller Boundary of XX, denoted RX\partial_{R}X, is the remainder space X¯X\bar{X}\setminus X. It is a fact that RX\partial_{R}X agrees with the collection of ultrafilters in X\mathcal{H}_{X}^{\circ} that do not satisfy the DCC. Note that an element ξRX\xi\in\partial_{R}X necessarily contains a nonterminating descending sequence. Of paramount interest to us is the case that ξ\xi contains a nonterminating descending sequence of strongly separated halfspaces, {𝔥i}\{{\mathfrak{h}}_{i}\}. We call such ξ\xi a regular point. These were originally defined in [Fer18] (and independently in [KS16]) as elements ξRX\xi\in\partial_{R}X such that if 𝔥1,𝔥2ξ{\mathfrak{h}}_{1},{\mathfrak{h}}_{2}\in\xi then there exists 𝔨X\mathfrak{k}\in\mathcal{H}_{X} with 𝔨𝔥1𝔥2\mathfrak{k}\subset{\mathfrak{h}}_{1}\cap{\mathfrak{h}}_{2} and 𝔨\mathfrak{k} is strongly separated from both 𝔥1{\mathfrak{h}}_{1} and 𝔥2{\mathfrak{h}}_{2}. They were also shown to be equivalent to the definition provided. [FLM18, Proposition 5.13] and Lemma 8 below imply that, if ξ\xi is a regular point containing a nonterminating descending sequence of strongly separated halfspaces, {𝔥i}\{{\mathfrak{h}}_{i}\}, and if ξ\xi^{\prime} is a regular point with {𝔥i}ξ\{{\mathfrak{h}}_{i}\}\subseteq\xi^{\prime} then ξ=ξ\xi^{\prime}=\xi. Due to this fact, we will often refer to a regular point, ξ\xi, simply as a nonterminating descending sequence of strongly separated halfspaces, {𝔥i}ξ\{{\mathfrak{h}}_{i}\}\subseteq\xi.

The visual boundary of a CAT(0) cube complex XX is the collection of equivalence classes of (CAT(0)) geodesic rays, where two such rays are equivalent if they remain within a bounded Hausdorff distance of each other. We denote the visual boundary by X\partial_{\infty}X.

2.4. Groups Acting on Cube Complexes

An element gIsom(X)g\in\operatorname{Isom}(X) is an automorphism if it acts as a cubical isomorphism of XX. We let Aut(X)\mathop{\mathrm{Aut}}\nolimits(X) denote the group of automorphisms of XX. A subgroup of Γ\Gamma in Aut(X)\mathop{\mathrm{Aut}}\nolimits(X) is said to act cocompactly if there exists a compact subcomplex KXK\leq X whose translates cover XX, i.e., X=ΓKX=\Gamma\cdot K. Under our assumption that XX is locally compact, this is equivalent to requiring that X/ΓX/\Gamma be compact. Γ\Gamma acts essentially if given any halfspace 𝔥{\mathfrak{h}} in XX, we have d(Γ𝔥^,𝔥^)d(\Gamma\cdot\hat{\mathfrak{h}},\hat{\mathfrak{h}}) is unbounded. Note that, for Γ\Gamma to act essentially, the halfspaces of XX must be deep.

For XX a CAT(0) cube complex, upon passing to its barycentric subdivision, elements gAut(X)g\in\mathop{\mathrm{Aut}}\nolimits(X) come in two types ([Hag07]):

  1. (1)

    (Elliptic) gg fixes a vertex in XX;

  2. (2)

    (Hyperbolic) gg is not elliptic and preserves a geodesic line.

A geodesic line preserved by gg is called an axis for gg. A rank one isometry is a hyperbolic automorphism gg none of whose axes bound a flat halfplane, and a contracting isometry is a rank one isometry with axis ll such that the diameter of the orthogonal projection to ll of any ball disjoint from ll is bounded above. An element in Aut(X)\mathop{\mathrm{Aut}}\nolimits(X) is regular if it acts as a contracting isometry on each irreducible factor of XX.

Contracting isometries can be detected by looking at their action on strongly separated hyperplanes. An element gAut(X)g\in\mathop{\mathrm{Aut}}\nolimits(X) is said to double skewer the pair of hyperplanes 𝔥^,𝔥^′′\hat{\mathfrak{h}}^{\prime},\hat{\mathfrak{h}}^{\prime\prime} if there is a nested pair of halfspaces 𝔥𝔥′′{\mathfrak{h}}^{\prime}\subset{\mathfrak{h}}^{\prime\prime} of XX such that 𝔥′′g𝔥{\mathfrak{h}}^{\prime\prime}\subsetneq g{\mathfrak{h}}^{\prime}.

Lemma 2 ([CS11]).

Let XX be a finite dimensional CAT(0)\operatorname{CAT(0)} cube complex and gAut(X)g\in\mathop{\mathrm{Aut}}\nolimits(X) double skewers a pair of strongly separated hyperplanes in XX. Then gg is a contracting isometry.

Suppose gAut(X)g\in\mathop{\mathrm{Aut}}\nolimits(X) double skewers (𝔥^,𝔥^′′)(\hat{\mathfrak{h}}^{\prime},\hat{\mathfrak{h}}^{\prime\prime}). Then for some choice of halfspace 𝔥{\mathfrak{h}}^{\prime} of the hyperplane 𝔥^\hat{\mathfrak{h}}^{\prime}, {gi𝔥}\{g^{i}{\mathfrak{h}}^{\prime}\} and {gi𝔥}\{g^{-i}{\mathfrak{h}}^{\prime*}\} give us two nonterminating descending sequence of halfspaces. Moreover, if 𝔥^\hat{\mathfrak{h}}^{\prime} and 𝔥^′′\hat{\mathfrak{h}}^{\prime\prime} are strongly separated hyperplanes, then both {gi𝔥}\{g^{i}{\mathfrak{h}}^{\prime}\} and {gi𝔥}\{g^{-i}{\mathfrak{h}}^{\prime*}\} are nonterminating descending sequences of strongly separated halfspaces, and hence correspond to two regular points in R(X)\partial_{R}(X). In this case gg can be thought as acting along an axis whose end points are {gi𝔥}\{g^{i}{\mathfrak{h}}^{\prime}\} and {gi𝔥}\{g^{-i}{\mathfrak{h}}^{\prime*}\}. We refer to {gi𝔥}\{g^{i}{\mathfrak{h}}^{\prime}\} and {gi𝔥}\{g^{-i}{\mathfrak{h}}^{\prime*}\} as poles of gg.

3. Girth Alternative for Lattices

One crucial step towards proving Girth Alternative is to find a sufficient condition for infinite girth. Recall that free groups have infinite girth. One classical way of producing a copy of free group on two generators as a subgroup in a given group Γ\Gamma is to use a version of the ping-pong lemma. This goes back to Tits [Tit72] where he proved the following.

Proposition 3 (Free subgroup criterion).

Let Γ\Gamma be a group acting on a set XX. Suppose there exist elements σ,τΓ\sigma,\tau\in\Gamma, subsets Uσ,UτXU_{\sigma},U_{\tau}\subset X, and a point xXx\in X, such that

  1. (1)

    xUσUτx\notin U_{\sigma}\cup U_{\tau}

  2. (2)

    σk({x}Uτ}Uσ\sigma^{k}(\{x\}\cup U_{\tau}\}\subset U_{\sigma} for all k{0}k\in\mathbb{Z}-\{0\}

  3. (3)

    τk({x}Uσ}Uτ\tau^{k}(\{x\}\cup U_{\sigma}\}\subset U_{\tau} for all k{0}k\in\mathbb{Z}-\{0\}.

Then σ,τ\langle\sigma,\tau\rangle is non-abelian free subgroup of Γ\Gamma.

However, mere containment of a copy of 𝔽2\mathbb{F}_{2} does not guarantee infinite girth. In fact, there exist groups with finite girth that have free non-abelian subgroups [Akh03]. Akhmedov [Akh05] observed that similar ping-pong arguments can be applied to certain classes of groups for which Tits Alternative holds to prove that a given group has infinite girth. Generalizing and reformulating the work of [Akh05], Nakamura obtained the following criterion for infinite girth in comparable generality to Proposition 3.

Theorem 4 (Criteria for infinite girth [Nak14], [Nak08]).

Let Γ\Gamma be a group acting on a set XX with a finite generating set S={γ1,,γn}S=\{\gamma_{1},\ldots,\gamma_{n}\}. Suppose there exist elements σ,τΓ\sigma,\tau\in\Gamma, subsets Uσ,UτXU_{\sigma},U_{\tau}\subset X, and a point xXx\in X such that

(1) x(UσUτ)ε=±1i=1nγiε(UσUτ)\displaystyle\;\;\;\;x\notin(U_{\sigma}\cup U_{\tau})\cup\bigcup_{\varepsilon=\pm 1}\bigcup_{i=1}^{n}\gamma_{i}^{\varepsilon}(U_{\sigma}\cup U_{\tau})
(2) σk({x}Uτε=±1i=1nγiε(Uτ))Uσforallk{0},and\displaystyle\;\;\;\;\sigma^{k}\left(\{x\}\cup U_{\tau}\cup\bigcup_{\varepsilon=\pm 1}\bigcup_{i=1}^{n}\gamma_{i}^{\varepsilon}(U_{\tau})\right)\subset U_{\sigma}\;\;for\;all\;k\in\mathbb{Z}-\{0\},\;and
(3) τk({x}Uσε=±1i=1nγiε(Uσ))Uτforallk{0}.\displaystyle\;\;\;\;\tau^{k}\left(\{x\}\cup U_{\sigma}\cup\bigcup_{\varepsilon=\pm 1}\bigcup_{i=1}^{n}\gamma_{i}^{\varepsilon}(U_{\sigma})\right)\subset U_{\tau}\;\;for\;all\;k\in\mathbb{Z}-\{0\}.

Then Γ\Gamma is a non-cyclic group with Girth(Γ)=\operatorname{Girth}(\Gamma)=\infty.

Clearly, the elements σ,τ\sigma,\tau and subsets Uσ,UτU_{\sigma},U_{\tau} in Theorem 4 satisfy the conditions in Proposition 3 and therefore σ,τΓ\langle\sigma,\tau\rangle\leq\Gamma must be a non-abelian free subgroup. In general, properties (2) and (3) can be interpreted as analogous to the North-South dynamics exhibited by the action of a loxodromic element in a hyperbolic group on its boundary. In the realm of irreducible CAT(0)\operatorname{CAT(0)} cube complexes, the role of such isometries are played by contracting isometries. In general, a finite dimensional CAT(0)\operatorname{CAT(0)} cube complex is a product of finitely many irreducible factors by Proposition 1. Therefore, to get infinite girth of a group acting on a finite dimensional CAT(0)\operatorname{CAT(0)} cube complex, we should look for isometries that act as contracting isometries when restricted to each irreducible factor. In other words, we are looking for regular elements.

The following Theorem of [CS11] says that regular elements always exist under certain conditions.

Theorem 5 (Regular elements in lattices [CS11]).

Let X=X1××XnX=X_{1}\times\ldots\times X_{n} be a product of irreducible, unbounded, locally compact CAT(0)\operatorname{CAT(0)} cube complexes such that Aut(Xi)\mathop{\mathrm{Aut}}\nolimits(X_{i}) acts cocompactly and essentially on XiX_{i} for each ii. Suppose that ΓAut(X)\Gamma\leq\mathop{\mathrm{Aut}}\nolimits(X) is a lattice (possible non-uniform). Suppose that 𝔥i𝔨i{\mathfrak{h}}_{i}\subset\mathfrak{k}_{i} are nested halfspaces in each factor XiX_{i}. Then there exists a regular element gΓg\in\Gamma which simultaneously double skewers these hyperplanes. That is to say, for each ii, g𝔨i𝔥ig\mathfrak{k}_{i}\subsetneq{\mathfrak{h}}_{i}.

The above Theorem reduces the problem of finding a regular element in ΓAut(X)\Gamma\leq\mathop{\mathrm{Aut}}\nolimits(X) to finding a pair of strongly separated hyperplanes in each irreducible factor of XX. For our purpose, we will need two such regular elements whose axes in each irreducible factor avoid certain points at infinity. In particular, we want their axes to not intersect at infinity in each irreducible factor. According to Theorem 5, if we can find a facing quadruple of hyperplanes in each irreducible factor XiX_{i}, each containing two pairs of strongly separated hyperplanes, then the group elements that skewer the strongly separated pairs in each XiX_{i} will have the desired property. Our next Lemma says that, under certain conditions, we always have such a collection of facing hyperplanes.

Warning on notations.

For the rest of the paper, the notation {ai,bi}\{a_{i},b_{i}\} will mean the set consisting of two elements aia_{i} and bib_{i} whereas the notation {ai}\{a_{i}\} will stand for a sequence {ai}i=1\{a_{i}\}_{i=1}^{\infty}. We will sometimes write sets with braces and at other times without braces, and we reserve parentheses for ordered sets.

Lemma 6 (Abundance of facing hyperplanes).

Let XX be an irreducible finite dimensional CAT(0)\operatorname{CAT(0)} cube complex where Aut(X)\mathop{\mathrm{Aut}}\nolimits(X) acts essentially and without fixed points at infinity. Let {𝔞^,𝔟^,𝔠^}\{\hat{\mathfrak{a}},\hat{\mathfrak{b}},\hat{\mathfrak{c}}\} be a facing triple in XX with 𝔞^\hat{\mathfrak{a}} and 𝔟^\hat{\mathfrak{b}} strongly separated. Then for any nn, there exists a collection of 2n2n facing hyperplanes {𝔞^1=𝔞^,𝔟^1=𝔟^,𝔞^2,𝔟^2,,𝔞^n,𝔟^n}\{\hat{\mathfrak{a}}_{1}=\hat{\mathfrak{a}},\hat{\mathfrak{b}}_{1}=\hat{\mathfrak{b}},\hat{\mathfrak{a}}_{2},\hat{\mathfrak{b}}_{2},\ldots,\hat{\mathfrak{a}}_{n},\hat{\mathfrak{b}}_{n}\} such that each pair {𝔞^i,𝔟^i}\{\hat{\mathfrak{a}}_{i},\hat{\mathfrak{b}}_{i}\} is strongly separated for all ii.

An automorphism gAut(X)g\in\mathop{\mathrm{Aut}}\nolimits(X) is said to flip a halfspace 𝔥{\mathfrak{h}}, if g𝔥𝔥g\cdot{\mathfrak{h}}\subsetneq{\mathfrak{h}}^{*}. The main idea of the proof of the above lemma is to hit one pair of hyperplanes from the triple by an automorphism that flips a halfspace corresponding to the third hyperplane, and then keep repeating this process on the resulting hyperplanes. The following Theorem of [CS11] says that any halfspace of XX can be flipped under certain conditions.

Theorem 7 (Flipping Lemma [CS11]).

Let XX be finite dimensional CAT(0)\operatorname{CAT(0)} cube complex and ΓAut(X)\Gamma\leq\mathop{\mathrm{Aut}}\nolimits(X) be a group acting essentially without a fixed point at infinity. Then for any halfspace 𝔥{\mathfrak{h}}, there is some γΓ\gamma\in\Gamma such that γ𝔥𝔥\gamma\cdot{\mathfrak{h}}\subsetneq{\mathfrak{h}}^{*}.

Proof of Lemma 6.

It is convenient to prove the lemma in terms of the halfspaces. Suppose (𝔞,𝔟,𝔠)({\mathfrak{a}},{\mathfrak{b}},{\mathfrak{c}}) is the facing triple of halfspaces. Let 𝔞1:=𝔞{\mathfrak{a}}_{1}:={\mathfrak{a}} and 𝔟1:=𝔟{\mathfrak{b}}_{1}:={\mathfrak{b}}. We start by applying an automorphism to the pair (𝔞1,𝔟1)({\mathfrak{a}}_{1},{\mathfrak{b}}_{1}) that flips the halfspace 𝔠{\mathfrak{c}}^{*} to get the pair (𝔞2,𝔟2)({\mathfrak{a}}_{2},{\mathfrak{b}}_{2}). Clearly the {𝔞1,𝔟1,𝔞2,𝔟2}\{{\mathfrak{a}}_{1},{\mathfrak{b}}_{1},{\mathfrak{a}}_{2},{\mathfrak{b}}_{2}\} are facing halfspaces and the pair {𝔞^2,𝔟^2}\{\hat{\mathfrak{a}}_{2},\hat{\mathfrak{b}}_{2}\} is strongly separated. By induction, suppose we have constructed the 2(n1)2(n-1) facing halfspaces {𝔞1,𝔟1,𝔞2,𝔟2,,𝔞n1,𝔟n1}\{{\mathfrak{a}}_{1},{\mathfrak{b}}_{1},{\mathfrak{a}}_{2},{\mathfrak{b}}_{2},\ldots,{\mathfrak{a}}_{n-1},{\mathfrak{b}}_{n-1}\} such that 𝔞^i\hat{\mathfrak{a}}_{i} and 𝔟^i\hat{\mathfrak{b}}_{i} are strongly separated for each ii where n2n\geq 2. To construct 2n2n facing hyperplanes, we apply an automorphism to the triple (𝔞1,𝔟1,𝔞n1)({\mathfrak{a}}_{1},{\mathfrak{b}}_{1},{\mathfrak{a}}_{n-1}) that flips 𝔟n1{\mathfrak{b}}^{*}_{n-1} to get (𝔞1,𝔟1,𝔞n1)({\mathfrak{a}}^{\prime}_{1},{\mathfrak{b}}^{\prime}_{1},{\mathfrak{a}}^{\prime}_{n-1}) and then apply another automorphism to the pair (𝔞1,𝔟1)({\mathfrak{a}}^{\prime}_{1},{\mathfrak{b}}^{\prime}_{1}) that flips 𝔞n1{\mathfrak{a}}^{\prime*}_{n-1} to get another pair (𝔞1′′,𝔟1′′)({\mathfrak{a}}^{\prime\prime}_{1},{\mathfrak{b}}^{\prime\prime}_{1}) [See figure 1]. By construction, {𝔞1,𝔟1}\{{\mathfrak{a}}^{\prime}_{1},{\mathfrak{b}}^{\prime}_{1}\} and {𝔞1′′,𝔟1′′}\{{\mathfrak{a}}^{\prime\prime}_{1},{\mathfrak{b}}^{\prime\prime}_{1}\} are both pairs of strongly separated hyperplanes. Finally, we claim that the collection {𝔞1,𝔟1,,𝔞n2,𝔟n2,𝔞1,𝔟1,𝔞1′′,𝔟1′′}\{{\mathfrak{a}}_{1},{\mathfrak{b}}_{1},\ldots,{\mathfrak{a}}_{n-2},{\mathfrak{b}}_{n-2},{\mathfrak{a}}^{\prime}_{1},{\mathfrak{b}}^{\prime}_{1},{\mathfrak{a}}^{\prime\prime}_{1},{\mathfrak{b}}^{\prime\prime}_{1}\} consists of facing halfspaces [Figure 1].

First, we observe that halfspaces in the collection {𝔞1,𝔟1,𝔞2′′,𝔟2′′}\{{\mathfrak{a}}_{1}^{\prime},{\mathfrak{b}}_{1}^{\prime},{\mathfrak{a}}^{\prime\prime}_{2},{\mathfrak{b}}^{\prime\prime}_{2}\} are mutually disjoint. This is because 𝔞1{\mathfrak{a}}_{1}^{\prime} and 𝔟1{\mathfrak{b}}_{1}^{\prime} are contained in 𝔞n1{\mathfrak{a}}^{\prime*}_{n-1}, and the pair (𝔞1′′,𝔟1′′)({\mathfrak{a}}^{\prime\prime}_{1},{\mathfrak{b}}^{\prime\prime}_{1}) is obtained by applying an automorphism to the pair (𝔞1,𝔟1)({\mathfrak{a}}^{\prime}_{1},{\mathfrak{b}}^{\prime}_{1}) that flips 𝔞n1{\mathfrak{a}}^{\prime*}_{n-1}. It follows that both 𝔞1′′{\mathfrak{a}}^{\prime\prime}_{1} and 𝔟1′′{\mathfrak{b}}^{\prime\prime}_{1} are contained inside 𝔞n1{\mathfrak{a}}^{\prime}_{n-1}. The claim follows. Next we show that both 𝔞1{\mathfrak{a}}^{\prime}_{1} and 𝔟1{\mathfrak{b}}^{\prime}_{1} are disjoint from the collection {𝔞1,𝔟1,,𝔞n2,𝔟n2}\{{\mathfrak{a}}_{1},{\mathfrak{b}}_{1},\ldots,{\mathfrak{a}}_{n-2},\newline {\mathfrak{b}}_{n-2}\}. By construction, (𝔞1,𝔟1)({\mathfrak{a}}^{\prime}_{1},{\mathfrak{b}}^{\prime}_{1}) is obtained by applying an automorphism to the pair (𝔞1,𝔟1)({\mathfrak{a}}_{1},{\mathfrak{b}}_{1}) that flips 𝔟n1{\mathfrak{b}}^{*}_{n-1}, therefore both 𝔞1{\mathfrak{a}}^{\prime}_{1} and 𝔟1{\mathfrak{b}}^{\prime}_{1} are contained inside 𝔟n1{\mathfrak{b}}_{n-1}. Since 𝔟n1{\mathfrak{b}}_{n-1} is disjoint from any set from the collection {𝔞1,𝔟1,,𝔞n2,𝔟n2}\{{\mathfrak{a}}_{1},{\mathfrak{b}}_{1},\ldots,{\mathfrak{a}}_{n-2},{\mathfrak{b}}_{n-2}\}, so are both 𝔞1{\mathfrak{a}}^{\prime}_{1} and 𝔟1{\mathfrak{b}}^{\prime}_{1}.

Similarly, we can show both 𝔞1′′{\mathfrak{a}}^{\prime\prime}_{1} and 𝔟1′′{\mathfrak{b}}^{\prime\prime}_{1} are disjoint from the collection {𝔞1,𝔟1,,𝔞n2,𝔟n2}\{{\mathfrak{a}}_{1},{\mathfrak{b}}_{1},\ldots,\newline {\mathfrak{a}}_{n-2},{\mathfrak{b}}_{n-2}\}. First note that, 𝔞n1𝔟n1{\mathfrak{a}}^{\prime}_{n-1}\subset{\mathfrak{b}}_{n-1} by construction. Also, 𝔞1′′𝔞n1{\mathfrak{a}}^{\prime\prime}_{1}\subset{\mathfrak{a}}^{\prime}_{n-1} and 𝔟1′′𝔞n1{\mathfrak{b}}^{\prime\prime}_{1}\subset{\mathfrak{a}}^{\prime}_{n-1}. Consequently both 𝔞1′′{\mathfrak{a}}^{\prime\prime}_{1} and 𝔟1′′{\mathfrak{b}}^{\prime\prime}_{1} are contained inside 𝔟n1{\mathfrak{b}}_{n-1} which is disjoint from any set from the collection {𝔞1,𝔟1,,𝔞n2,𝔟n2}\{{\mathfrak{a}}_{1},{\mathfrak{b}}_{1},\ldots,{\mathfrak{a}}_{n-2},{\mathfrak{b}}_{n-2}\}. This finishes the proof. ∎

𝔞^1\displaystyle\hat{\mathfrak{a}}_{1}𝔟^1\displaystyle\hat{\mathfrak{b}}_{1}𝔞^n1\displaystyle\hat{\mathfrak{a}}_{n-1}𝔟^n1\displaystyle\hat{\mathfrak{b}}_{n-1}𝔞^n1\displaystyle\hat{\mathfrak{a}}^{\prime}_{n-1}𝔞^1′′\displaystyle\hat{\mathfrak{a}}^{\prime\prime}_{1}𝔟^1′′\displaystyle\hat{\mathfrak{b}}^{\prime\prime}_{1}𝔞^1\displaystyle\hat{\mathfrak{a}}^{\prime}_{1}𝔟^1\displaystyle\hat{\mathfrak{b}}^{\prime}_{1}
Figure 1. The above picture shows how to increase the number of facing hyperplanes. The input is four facing hyperplanes {𝔞^1,𝔟^1,𝔞^n1,𝔟^n1}\{\hat{\mathfrak{a}}_{1},\hat{\mathfrak{b}}_{1},\hat{\mathfrak{a}}_{n-1},\hat{\mathfrak{b}}_{n-1}\} and the output is six facing hyperplanes {𝔞^1,𝔟^1,𝔞^1,𝔟^1,𝔞^1′′,𝔟^1′′}\{\hat{\mathfrak{a}}_{1},\hat{\mathfrak{b}}_{1},\hat{\mathfrak{a}}^{\prime}_{1},\hat{\mathfrak{b}}^{\prime}_{1},\hat{\mathfrak{a}}^{\prime\prime}_{1},\hat{\mathfrak{b}}^{\prime\prime}_{1}\}.

As mentioned before, we need to find two regular elements whose axis in each irreducible factor do not intersect each other at infinity. More precisely, we want the poles of these two elements to be ‘disjoint’ from each other in each factor. Recall that poles are defined in terms of descending sequences of half spaces. We say, two descending sequences of half spaces {Pn}\{P_{n}\} and {Qn}\{Q_{n}\} are disjoint if PmQm=P_{m}\cap Q_{m}=\emptyset for some mm. Otherwise, we say that {Pn}\{P_{n}\} and {Qn}\{Q_{n}\} intersects each other. The next lemma shows that a descending sequence of strongly separated halfspaces cannot intersect two disjoint descending sequence of halfspaces simultaneously. The statement and its proof are similar to [FLM18, Lemma 5.11], but somewhat different, so we include them for the convenience of the reader.

Lemma 8 (Disjoint descending sequence of halfspaces).

Let {𝔞n}\{{\mathfrak{a}}_{n}\} and {𝔟n}\{{\mathfrak{b}}_{n}\} be two disjoint descending sequence of halfspaces in a finite dimensional CAT(0)\operatorname{CAT(0)} cube complex XX. Let {𝔠n}\{{\mathfrak{c}}_{n}\} be another descending sequence of strongly separated halfspaces in XX that intersects {𝔞n}\{{\mathfrak{a}}_{n}\}. Then {𝔠n}\{{\mathfrak{c}}_{n}\} and {𝔟n}\{{\mathfrak{b}}_{n}\} are disjoint.

Proof.

We need to show that 𝔟n𝔠n={\mathfrak{b}}_{n}\cap{\mathfrak{c}}_{n}=\emptyset for sufficiently large nn. By hypothesis, there exist NN such that 𝔞i𝔟i={\mathfrak{a}}_{i}\cap{\mathfrak{b}}_{i}=\emptyset for all iNi\geq N. Since {𝔠n}\{{\mathfrak{c}}_{n}\} is descending and intersects {𝔞n}\{{\mathfrak{a}}_{n}\}, there exists MM such that 𝔞N𝔠M{\mathfrak{a}}_{N}\cap{\mathfrak{c}}_{M}\neq\emptyset. So, either 𝔠M𝔞N{\mathfrak{c}}_{M}\subset{\mathfrak{a}}_{N}, or 𝔠M𝔞N{\mathfrak{c}}^{*}_{M}\subset{\mathfrak{a}}_{N} or 𝔠^M𝔞^N\hat{\mathfrak{c}}_{M}\pitchfork\hat{\mathfrak{a}}_{N}.

Next, we will show how to rule out the second and third cases by taking MM large enough. To rule out the second case, we observe that 𝔠M𝔠M+k𝔞N{\mathfrak{c}}^{*}_{M}\subset{\mathfrak{c}}^{*}_{M+k}\subset{\mathfrak{a}}_{N} for all k0k\geq 0. However, since XX is finite dimensional, there can be at most finitely many hyperplanes between any two halfspaces. So, for large enough MM, the second case does not occur. To rule out the third case, suppose 𝔠^M𝔞^N\hat{\mathfrak{c}}_{M}\pitchfork\hat{\mathfrak{a}}_{N} for some MM. Since 𝔠M{\mathfrak{c}}_{M} and 𝔠M+1{\mathfrak{c}}_{M+1} are strongly separated, 𝔞N{\mathfrak{a}}_{N} cannot be transverse to 𝔠M+1{\mathfrak{c}}_{M+1}. So, either 𝔞N𝔠M+1={\mathfrak{a}}_{N}\cap{\mathfrak{c}}_{M+1}=\emptyset or 𝔠M+1𝔞N{\mathfrak{c}}_{M+1}\subset{\mathfrak{a}}_{N}. By hypothesis 𝔞N𝔠M+1{\mathfrak{a}}_{N}\cap{\mathfrak{c}}_{M+1}\neq\emptyset. Therefore, we have 𝔠M+1𝔞N{\mathfrak{c}}_{M+1}\subset{\mathfrak{a}}_{N}.

So we are left with the first possibility which is 𝔠M𝔞N{\mathfrak{c}}_{M}\subset{\mathfrak{a}}_{N} for some MM. Since 𝔞N𝔟N={\mathfrak{a}}_{N}\cap{\mathfrak{b}}_{N}=\emptyset, it follows that 𝔠M𝔟N={\mathfrak{c}}_{M}\cap{\mathfrak{b}}_{N}=\emptyset. Since the sequences of halfspaces are descending, we get {𝔠n}\{{\mathfrak{c}}_{n}\} is disjoint from {𝔟n}\{{\mathfrak{b}}_{n}\}. ∎

We say that a CAT(0)\operatorname{CAT(0)} cube complex XX is 𝐑\operatorname{\bf{R}}-like if there is an Aut(X)\mathop{\mathrm{Aut}}\nolimits(X)-invariant geodesic line in XX. The final ingredient to our main theorem is the following Lemma which characterizes cube complexes with invariant Euclidean flats.

Lemma 9 ([CS11]).

Let XX be a finite dimensional CAT(0)\operatorname{CAT(0)} cube complex such that Aut(X)\mathop{\mathrm{Aut}}\nolimits(X) acts essentially. Then Aut(X)\mathop{\mathrm{Aut}}\nolimits(X) stabilizes some nn-dimensional flat 𝐑nX\operatorname{\bf{R}}^{n}\subset X if and only if XX decomposes as a product X=X1×X2××XnX=X_{1}\times X_{2}\times\ldots\times X_{n} of subcomplexes, each of which is essential and 𝐑\operatorname{\bf{R}}-like.

We are now ready to prove our main theorem which appears as Theorem C in the introduction.

Theorem 10 (Girth Alternative for lattices, version 1).

Let X=X1××XnX=X_{1}\times\dots\times X_{n} be a product of nn irreducible, unbounded, locally compact CAT(0)\operatorname{CAT(0)} cube complexes such that Aut(Xi)\mathop{\mathrm{Aut}}\nolimits(X_{i}) acts cocompactly and essentially on XiX_{i} for all ii.

Then for any (possibly non-uniform) lattice ΓAut(X)\Gamma\leq\mathop{\mathrm{Aut}}\nolimits(X), either Γ\Gamma virtually fixes some point in XXX\cup\partial_{\infty}X or Girth(Γ)=\operatorname{Girth}(\Gamma)=\infty.

Proof.

Suppose ΓAut(X)\Gamma\leq\mathop{\mathrm{Aut}}\nolimits(X) does not fix a point in XXX\cup\partial_{\infty}X. We want to show that Girth(Γ)=\operatorname{Girth}(\Gamma)=\infty.

Since Γ\Gamma does not have fixed points at infinity, Aut(X)\mathop{\mathrm{Aut}}\nolimits(X) does not have fixed points at infinity. Furthermore, since Aut(X)\mathop{\mathrm{Aut}}\nolimits(X) acts essentially on XX, we can invoke [CS11, Proposition 5.1] to obtain a pair of strongly separated hyperplane {𝔥^i,𝔡^i}\{\hat{\mathfrak{h}}_{i},\hat{\mathfrak{d}}_{i}\} in each XiX_{i}.

We now apply Theorem 5 to obtain an element σΓ\sigma\in\Gamma that double skewers (𝔥^i,𝔡^i)(\hat{\mathfrak{h}}_{i},\hat{\mathfrak{d}}_{i}) in each XiX_{i}. Let 𝔥i{\mathfrak{h}}_{i} be the halfspace corresponding to the hyperplane 𝔥^i\hat{\mathfrak{h}}_{i} such that σj+1𝔥iσj𝔥i\sigma^{j+1}{\mathfrak{h}}_{i}\subset\sigma^{j}{\mathfrak{h}}_{i} for any jj\in\mathbb{N}. Since (𝔥^i,𝔡^i)(\hat{\mathfrak{h}}_{i},\hat{\mathfrak{d}}_{i}) are strongly separated hyperplanes, it follows that {σn𝔥i}\{\sigma^{n}{\mathfrak{h}}_{i}\} and {σn𝔥i}\{\sigma^{-n}{\mathfrak{h}}^{*}_{i}\} are two disjoint descending sequence of strongly separated halfspaces. In other words, they are the poles of σ\sigma in XiX_{i} (see preliminaries).

Next, we choose an arbitrary generating set {γ1,γ2,,γk}\{\gamma_{1},\gamma_{2},\ldots,\gamma_{k}\} of Γ\Gamma. We will consider the translate of poles of σ\sigma in each XiX_{i} under this generating set. More precisely, we consider the following list of descending sequences of halfspaces:

(\dagger) {σn𝔥i},{σn𝔥i},{γjσn𝔥i},{γjσn𝔥i},{γj1σn𝔥i},{γj1σn𝔥i}\{\sigma^{n}{\mathfrak{h}}_{i}\},\{\sigma^{-n}{\mathfrak{h}}_{i}^{*}\},\{\gamma_{j}\sigma^{n}{\mathfrak{h}}_{i}\},\{\gamma_{j}\sigma^{-n}{\mathfrak{h}}^{*}_{i}\},\{\gamma_{j}^{-1}\sigma^{n}{\mathfrak{h}}_{i}\},\{\gamma_{j}^{-1}\sigma^{-n}{\mathfrak{h}}_{i}^{*}\}

where 1in1\leq i\leq n and 1jk1\leq j\leq k. Since isometries preserve strong separation, all the sequences in the above list consists of strongly separated halfspaces.

(Also note that, for a fix ii, all the halfspaces in the above list may not live in XiX_{i}, because γj\gamma_{j} can switch isomorphic factors. However, they all live in some XiX_{i}).

Now, we are going to produce another regular element τΓ\tau\in\Gamma such that the poles in each XiX_{i} are disjoint from the list (\dagger3). In particular, its poles will be disjoint from that of σ\sigma. This is where we are going to use the fact that Γ\Gamma does not fix a point in XXX\cup\partial_{\infty}X. This will ensure that each XiX_{i} is large, in a certain sense. More precisely, we will see that each XiX_{i} has a facing triple.

First we observe that, since each XiX_{i} is finite dimensional and locally compact and Aut(Xi)\mathop{\mathrm{Aut}}\nolimits(X_{i}) acts essentially and cocompactly on XiX_{i}, by [CS11, Theorem 7.2], either Aut(Xi)\mathop{\mathrm{Aut}}\nolimits(X_{i}) stabilizes some Euclidean flat or there is a facing triple of hyperplanes in XiX_{i}.

Suppose Aut(Xi)\mathop{\mathrm{Aut}}\nolimits(X_{i}) stabilizes some Euclidean flat FiXiF_{i}\subset X_{i}. Since XiX_{i} is irreducible, it follows from Lemma 9 that FiF_{i} is R-like. Thus Aut(Xi)\mathop{\mathrm{Aut}}\nolimits(X_{i}) has an index two subgroup which fixes a point at infinity contradicting our assumption on Γ\Gamma. Therefore, we have a facing triple of hyperplanes in each XiX_{i}. Moreover, we can choose this facing triple in a way so that there is a pair of hyperplanes in the triple that are strongly separated (see the proof of [CS11, Theorem 7.2] for details).

By Lemma 6, there exist infinitely many pairs of strongly separated hyperplanes in each XiX_{i} that are facing each other. Given a pair of strongly separated hyperplanes taken from each XiX_{i}, we can choose an element from Γ\Gamma that double skewers each pair in the corresponding XiX_{i} due to Theorem 5. Since all the pairs are facing each other, the poles of these group elements give us infinitely many mutually disjoint descending sequence of strongly separated hyperplanes in XiX_{i}. Of these infinitely many descending sequences of halfspaces in XiX_{i}, all but finitely many are disjoint from the list (\dagger3) by Lemma 8 because the list (\dagger3) contains a finite number of descending sequences of strongly separated halfspaces. In particular, there exists a pair of disjoint halfspaces {𝔥i,𝔡i}\{{\mathfrak{h}}^{\prime}_{i},\mathfrak{d}^{\prime}_{i}\} in each XiX_{i}, such that for large enough NN, both 𝔥i{\mathfrak{h}}^{\prime}_{i} and 𝔡i\mathfrak{d}^{\prime}_{i} are disjoint from the following collection

{σN𝔥i,σN𝔥i,γjσN𝔥i,γjσN𝔥i,γj1σN𝔥i,γj1σN𝔥i1in,1jk}.\bigl{\{}\sigma^{N}{\mathfrak{h}}_{i},\sigma^{-N}{\mathfrak{h}}_{i},\gamma_{j}\sigma^{N}{\mathfrak{h}}_{i}^{*},\gamma_{j}\sigma^{-N}{\mathfrak{h}}^{*}_{i},\gamma_{j}^{-1}\sigma^{N}{\mathfrak{h}}_{i},\gamma_{j}^{-1}\sigma^{-N}{\mathfrak{h}}_{i}^{*}\mid 1\leq i\leq n,1\leq j\leq k\bigr{\}}.

Let τΓ\tau\in\Gamma be an element that double skewers (𝔥^i,𝔡^i)(\hat{\mathfrak{h}}^{\prime}_{i},\hat{\mathfrak{d}}^{\prime}_{i}) in each XiX_{i}. Without loss of generality, let us assume that {τn𝔥i}\{\tau^{n}{\mathfrak{h}}^{\prime}_{i}\} and {τn𝔥i}\{\tau^{-n}{\mathfrak{h}}^{\prime*}_{i}\} are the poles of τ\tau in XiX_{i}.

We let Y:=i=1nXiY:=\sqcup_{i=1}^{n}X_{i}. Note that Γ\Gamma acts on YY. We set Uσ:=i(σN𝔥iσN𝔥i)U_{\sigma^{\prime}}:=\bigcup_{i}(\sigma^{N}{\mathfrak{h}}_{i}\cup\sigma^{-N}{\mathfrak{h}}_{i}^{*}) and Uτ:=i(τN𝔥iτN𝔥i)U_{\tau^{\prime}}:=\bigcup_{i}(\tau^{N}{\mathfrak{h}}^{\prime}_{i}\cup\tau^{-N}{\mathfrak{h}}^{\prime*}_{i}).

Note that, the complement of σN𝔥iσN𝔥i\sigma^{N}{\mathfrak{h}}_{i}\cup\sigma^{-N}{\mathfrak{h}}_{i}^{*} in XiX_{i} get sent to σN𝔥iσN𝔥i\sigma^{N}{\mathfrak{h}}_{i}\cup\sigma^{-N}{\mathfrak{h}}_{i}^{*} under high enough power of σ±1\sigma^{\pm 1}. Taking union over ii, we obtain that complement of UσU_{\sigma} in YY get sent to UσU_{\sigma} under high enough power of σ±1\sigma^{\pm 1}. Similarly, complement of UτU_{\tau} in YY get sent to UτU_{\tau} under high enough power of τ±1\tau^{\pm 1}. We set σ=σM\sigma^{\prime}=\sigma^{M}, τ=τM\tau^{\prime}=\tau^{M}, where we choose MM so large that for all i{0}i\in\mathbb{Z}-\{0\}, we have

(11) (σ)i(YUσ)Uσ and (τ)i(YUτ)Uτ(\sigma^{\prime})^{i}(Y-U_{\sigma^{\prime}})\subset U_{\sigma^{\prime}}\quad\text{ and }\quad(\tau^{\prime})^{i}(Y-U_{\tau^{\prime}})\subset U_{\tau^{\prime}}

Next, we observe that, by construction, UσU_{\sigma^{\prime}} and its translates under the generating set and their inverses do not intersect UτU_{\tau^{\prime}}. In other words we have,

(22) Uσϵ=±1j=1kγjϵ(Uσ)YUτ.U_{\sigma^{\prime}}\cup\bigcup_{\epsilon=\pm 1}\bigcup_{j=1}^{k}\gamma_{j}^{\epsilon}(U_{\sigma^{\prime}})\subset Y-U_{\tau^{\prime}}.

Since γj(Uσ)Uτ=\gamma_{j}(U_{\sigma^{\prime}})\cap U_{\tau^{\prime}}=\emptyset iff γj1(Uτ)Uσ=\gamma^{-1}_{j}(U_{\tau^{\prime}})\cap U_{\sigma^{\prime}}=\emptyset for any γj\gamma_{j}, it follows from (22) that UτU_{\tau^{\prime}} and its translates under the generating set and their inverses do not intersect UσU_{\sigma^{\prime}}. In other words, we have

(33) Uτϵ=±1j=1kγjϵ(Uτ)YUσU_{\tau^{\prime}}\cup\bigcup_{\epsilon=\pm 1}\bigcup_{j=1}^{k}\gamma_{j}^{\epsilon}(U_{\tau^{\prime}})\subset Y-U_{\sigma^{\prime}}

Furthermore, we can assume (by taking NN large enough) that the following set

YUσUτε=±1j=1kγjε(UσUτ)Y-U_{\sigma^{\prime}}\cup U_{\tau^{\prime}}\cup\bigcup_{\varepsilon=\pm 1}\bigcup_{j=1}^{k}\gamma_{j}^{\varepsilon}(U_{\sigma^{\prime}}\cup U_{\tau^{\prime}})

is nonempty and for convenience, let us call this set BB.

We claim that σ,τ,Uσ,Uτ\sigma^{\prime},\tau^{\prime},U_{\sigma^{\prime}},U_{\tau^{\prime}}, and any point xBx\in B satisfies the three properties of Lemma 4.

The first property is immediate by our choice of xx. To check the second property, note that xYUσx\in Y-U_{\sigma^{\prime}} and together with (33) this implies

{x}Uτϵ=±1j=1kγjϵ(Uτ)YUσ\{x\}\cup U_{\tau^{\prime}}\cup\bigcup_{\epsilon=\pm 1}\bigcup_{j=1}^{k}\gamma_{j}^{\epsilon}(U_{\tau^{\prime}})\subset Y-U_{\sigma^{\prime}}

Therefore, (11) gives us

(σ)i({x}Uτϵ=±1j=1kγjϵ(Uτ))Uσfor all i{0}(\sigma^{\prime})^{i}(\{x\}\cup U_{\tau^{\prime}}\cup\bigcup_{\epsilon=\pm 1}\bigcup_{j=1}^{k}\gamma_{j}^{\epsilon}(U_{\tau^{\prime}}))\subset U_{\sigma^{\prime}}\quad\text{for all }i\in\mathbb{Z}-\{0\}

which is the desired second property.

Similarly, xYUτx\in Y-U_{\tau^{\prime}}, together with (22) and (11) gives us

(τ)i({x}Uσϵ=±1j=1kγjϵ(Uσ))Uτ(\tau^{\prime})^{i}(\{x\}\cup U_{\sigma^{\prime}}\cup\bigcup_{\epsilon=\pm 1}\bigcup_{j=1}^{k}\gamma_{j}^{\epsilon}(U_{\sigma^{\prime}}))\subset U_{\tau^{\prime}}

which is the desired third property.

Therefore, Girth(Γ)=\operatorname{Girth}(\Gamma)=\infty by Theorem 4. ∎

We will now prove the following version of Girth Alternative. The statement and its proof are inspired by [CS11, Corollary G].

Theorem 11 (Girth Alternative for lattices, version 2).

Let X=X1××XnX=X_{1}\times\dots\times X_{n} be a product of nn irreducible, unbounded, and locally compact CAT(0)\operatorname{CAT(0)} cube complexes such that Aut(Xi)\mathop{\mathrm{Aut}}\nolimits(X_{i}) acts cocompactly and essentially on XiX_{i} for all ii.

Then for any (possibly non-uniform) lattice ΓAut(X)\Gamma\leq\mathop{\mathrm{Aut}}\nolimits(X) acting properly on XX, either Γ\Gamma is {locally finite}-by-{virtually abelian} or Girth(Γ)=\operatorname{Girth}(\Gamma)=\infty.

The proof of the above will rely on the proof of Theorem 10 and a result of [CL10]. In addition, we will need the following lemmas to equivariantly triangulate certain subcomplexes in XX.

Lemma 12.

Suppose GG acts by automorphism on a locally finite cube complex XX. Suppose YXY\subset X be a GG-invariant subset and GG does not fix YY point-wise. Then there exists pYp\in Y such that

k:=inf{d(p,gp)gG,pgp}>0k:=\inf\{d(p,g\cdot p)\mid g\in G,p\neq g\cdot p\}>0
Proof.

By the assumption, we can choose pYp\in Y such that gppg\cdot p\neq p for some gGg\in G. Now we have two cases to consider.

Suppose pp is a vertex in XX. Since GG acts by automorphisms, translates of pp can only be other vertices. It follows that kk is at least the minimum of the distances between pp and other vertices. Since XX is locally finite, it follows that k>0k>0.

If pp is not a vertex, then pp is in the interior of some cube CC in XX. The infimum of distances between pp and all the translates of pp that are inside a different cube is clearly positive. Since there are only finitely many automophisms of CC, there are only finitely many nontrivial translates of pp that stay inside CC. Therefore the minimum distance from pp to any of its translates inside CC is also positive. The claim follows. ∎

Lemma 13.

Suppose GG acts on \mathbb{R} by isometries such that for some pp

k:=inf{d(p,gp)gG,pgp}>0.k:=\inf\{d(p,g\cdot p)\mid g\in G,p\neq g\cdot p\}>0.

Then there exists a finite index subgroup of HH and an HH-equivariant triangulation of \mathbb{R}.

Proof.

Let HH be the index two subgroup of GG consisting of only the orientation preserving isometries. In particular, HH acts by translation on \mathbb{R} and hence is a subgroup of \mathbb{R}. Either HH is trivial or k>0k>0 implies that

k:=inf{d(p,hp)hH,php}>0k^{\prime}:=\inf\{d(p,h\cdot p)\mid h\in H,p\neq h\cdot p\}>0

It follows that HH is generated by the isometry that translates by kk^{\prime} amount. Therefore, placing the vertices at integer multiples of kk^{\prime}, we obtain a HH-equivariant triangulation of \mathbb{R}. ∎

Combining the above two lemmas we immediately get the following.

Lemma 14.

Suppose GG acts by automorphisms on a locally finite 𝐑\operatorname{\bf{R}}-like cube complex XX and let LXL\subset X be an Aut(X)\mathop{\mathrm{Aut}}\nolimits(X)-invariant bi-infinite geodesic in XX. Then there exists a finite index subgroup HH of GG and a HH-equivariant triangulation of LL.

Proof.

If GG fixes LL pointwise, then any triangulation of LL is GG-equivariant. Otherwise, we can apply Lemma 12 with Y:=LY:=L to conclude that kk as in Lemma 12 is positive. Therefore we can apply Lemma 13 to LL which yields a finite index subgroup HH of GG and an HH-equivariant triangulation of LL. ∎

Proof of Theorem 11.

It follows from [CL10, Theorem 1.7] that Γ\Gamma is {locally finite}-by-{virtually abelian} if and only if Γ\Gamma is amenable. Thus it is enough to show that if Γ\Gamma is not amenable, then Girth(Γ)=\operatorname{Girth}(\Gamma)=\infty. Suppose Γ\Gamma is non-amenable. We claim there is an irreducible factor of XX that is not 𝐑\operatorname{\bf{R}}-like.

If each irreducible factor of XX is 𝐑\operatorname{\bf{R}}-like, then we can take the Aut(Xi)\mathop{\mathrm{Aut}}\nolimits(X_{i})-invariant geodesic in each factor and take their product to get an invariant nn-dimensional Euclidean flat. Let Γ\Gamma^{\prime} be the finite index subgroup of Γ\Gamma that stabilizes each factor. In particular, Γ\Gamma^{\prime} stabilizes the bi-infinite geodesic lines in each factor. Applying Lemma 14 to the action of Γ\Gamma^{\prime} on each 𝐑\operatorname{\bf{R}}-like factor, we get a finite index subgroup of Γ\Gamma^{\prime} which acts by automorphisms on some triangulation of the bi-infinite geodesic line in that 𝐑\operatorname{\bf{R}}-like factor. Taking the intersection of all these finite index subgroup for each factor we get another finite index subgroup Γ′′Γ\Gamma^{\prime\prime}\leq\Gamma^{\prime} that acts by automorphisms on each triangulated geodesic line. Γ′′\Gamma^{\prime\prime} therefore acts by automorphisms on a Euclidean flat YY where YY is the product of triangulated geodesic lines. By [Gen22, Lemma 2.8], the set of bounded components in the Roller boundary of YY is finite and nonempty. These bounded components have cubical structure that is respected by the induced action of Γ′′\Gamma^{\prime\prime}. Furthermore, the action of Γ′′\Gamma^{\prime\prime} stabilizes the union of these bounded components. In particular, Γ′′\Gamma^{\prime\prime} stabilizes some finite set of vertices in the Roller boundary and consequently a finite index subgroup of Γ′′\Gamma^{\prime\prime} fixes a point in the Roller boundary of YY. By [CL11, Theorem A.5], Γ′′\Gamma^{\prime\prime} is amenable. Since Γ′′Γ\Gamma^{\prime\prime}\leq\Gamma is a finite index subgroup, Γ\Gamma is amenable. This is a contradiction.

Hence at least one irreducible factor of XX is not 𝐑\operatorname{\bf{R}}-like, and hence contains a facing triple by [CS11, Theorem 7.2]. Now, we can discard all the 𝐑\operatorname{\bf{R}}-like factors from XX to get a space YY such that each irreducible factor of YY has a facing triple. Now we can run the same argument as in Theorem 10 to conclude that the girth of Γ\Gamma is infinite. ∎

Remark 15.

In our Girth Alternative theorems, we require the group to be a lattice in Aut(X)\mathop{\mathrm{Aut}}\nolimits(X) whereas the analogous Tits Alternative theorems of Caprace–Sageev [CS11] (also see [SW05]) do not require the group to be a lattice. The main reason for the lattice assumption in our case is that we need regular elements that double skewer a given pair of hyperplanes in each irreducible factor to obtain infinite girth. And Theorem 5 of [CS11] gives us such elements for lattices. Whereas, in the proof of Tits Alternative, one needs to find a free subgroup. In this case, we only need two group elements that double skewer distinct pairs of hyperplanes in some irreducible factor (see [CS11] for details). Interestingly, authors in [FLM18, Theorem 1.5] proved that regular elements exist whenever the group acts essentially and without fixed points in XXX\cup\partial_{\infty}X. Moreover, the group does not need to be a lattice in order to contain regular elements. This suggests that the lattice assumption may be dropped from Theorem 10. However, we do not know how to use the probabilistic methods of [FLM18] to produce an abundance of regular elements concretely without the lattice assumption.

Remark 16.

Another way of getting rid of the lattice assumption is the following. Note that Γ\Gamma has a finite index subgroup Γ\Gamma^{\prime} that stabilizes each irreducible factor factor by Proposition 1. With that in mind, we can run the same argument as in Theorem 10, but only working with the Γ\Gamma^{\prime}-action on X1X_{1} to prove that either Γ\Gamma virtually fixes a point or Girth(Γ)=\operatorname{Girth}(\Gamma^{\prime})=\infty without assuming Γ\Gamma to be lattice: since we can forget about the other factors, we only need σ\sigma and τ\tau to act as contracting isometries on X1X_{1}, and such elements always exist without the lattice assumption by [CS11]. So, another way to remove the lattice assumption in Theorem 10 would be to show that Girth(Γ)=\operatorname{Girth}(\Gamma^{\prime})=\infty implies Girth(Γ)=\operatorname{Girth}(\Gamma)=\infty. Although it seems plausible, we do not know whether containing a finite index subgroup with infinite girth is enough to guarantee the group itself has infinite girth.

4. Curious Examples

As promised in the introduction, we construct spaces which are R-like with particular group actions showing that Corollary B does not hold if both the assumptions properness and having a bound on the order of finite subgroups are omitted.

For a cube complex XX, we call a pair of vertices v,vXv,v^{*}\in X diametrically opposed if there exists a labeling of the halfspaces of XX so that θ(v)={𝔥|𝔥^^}\theta(v)=\{{\mathfrak{h}}\;|\;\hat{{\mathfrak{h}}}\in\hat{\mathcal{H}}\} and θ(v)={𝔥|𝔥^^}\theta(v^{*})=\{{\mathfrak{h}}^{*}\;|\;\hat{{\mathfrak{h}}}\in\hat{\mathcal{H}}\}. Note that a CAT(0) cube complex XX contains diametrically opposed vertices if and only if there is a geodesic path between vertices that crosses every hyperplane in XX.

If XX and YY are CAT(0) cube complexes each containing a pair of diametrically opposed vertices, then their product X×YX\times Y will contain a pair of diametrically opposed vertices. Indeed, if {𝔥i}\{{\mathfrak{h}}_{i}\} and {𝔥i}\{{\mathfrak{h}}_{i}^{*}\} define vertices x,xXx,x^{*}\in X, and {𝔨i}\{\mathfrak{k}_{i}\} and {𝔨i}\{\mathfrak{k}_{i}^{*}\} define vertices y,yYy,y^{*}\in Y, then (x,y)(x,y) and (x,y)(x^{*},y^{*}) give diametrically opposed vertices in X×YX\times Y.

Definition 17 (Cube Complex [X]\mathcal{L}{[X]}).

Begin with a CAT(0) cube complex XX which contains diametrically opposed vertices vv and vv^{*}. For all ii\in\mathbb{Z}, let XiX_{i} be an isomorphic copy of XX, where viv_{i} and viv_{i}^{*} denote the images of vv and vv^{*}, respectively. The cube complex [X]\mathcal{L}[X] is then formed by identifying viv_{i}^{*} with vi+1v_{i+1} for all ii\in\mathbb{Z}. We think of [X]\mathcal{L}[X] informally as a “line of XX’s.”

The space [X]\mathcal{L}[X] is clearly a cube complex as the map attaching distinct copies of XX is an isometry of vv. That [X]\mathcal{L}[X] is locally CAT(0) is also clear, since the link of a vertex labeled vv (or vv^{*}) in [X]\mathcal{L}[X] is isomorphic to the disjoint union of two copies of the link of vv in XX. Lastly, [X]\mathcal{L}[X] is simply-connected by construction.

There is a natural action of \mathbb{Z} on [X]\mathcal{L}[X] whereby each copy XX is shifted to an adjacent copy. With Autv,v(X)Aut(X)\mathop{\mathrm{Aut}}\nolimits_{v,v^{*}}(X)\leq\mathop{\mathrm{Aut}}\nolimits(X) denoting the automorpisms fixing both vv and vv^{*}, ΣX=Autv,v(X)\Sigma_{X}=\oplus\mathop{\mathrm{Aut}}\nolimits_{v,v^{*}}(X) acts on [X]\mathcal{L}[X] by allowing only finitely many coordinate groups to act nontrivially at a time. Clearly ΣX\mathbb{Z}\cap\Sigma_{X} is the identity element. We are interested in the semi-direct product ΣXAutv,v(X)\mathbb{Z}\ltimes\Sigma_{X}\cong\mathop{\mathrm{Aut}}\nolimits_{v,v^{*}}(X)\wr\mathbb{Z}, where multiplication is defined as (σ1,τm)(σ2,τn)=(σ1τmσ2τm,τm+n)(\sigma_{1},\tau^{m})(\sigma_{2},\tau^{n})\;=\;(\sigma_{1}\tau^{m}\sigma_{2}\tau^{-m},\tau^{m+n}) and (σ,τn)1=(τnσ1τn,τn)(\sigma,\tau^{n})^{-1}=(\tau^{-n}\sigma^{-1}\tau^{n},\tau^{-n}). Note that ΣX\mathbb{Z}\ltimes\Sigma_{X} is generated by the group Autv,v(X)\mathop{\mathrm{Aut}}\nolimits_{v,v^{*}}(X) and a single shift.

We define a group action of ΣX\mathbb{Z}\ltimes\Sigma_{X} on [X]\mathcal{L}[X] by

(σ,τn)(x)=στn(x)(\sigma,\tau^{n})\cdot(x)\;=\;\sigma\tau^{n}\cdot(x)

This action is faithful since (σ,τn)(\sigma,\tau^{n}) acts trivially if and only if both σ\sigma and τ\tau are the identity element in ΣX\Sigma_{X} and \mathbb{Z}, respectively. Since it acts faithfully, there is an injective map ΣXAut([X])\mathbb{Z}\ltimes\Sigma_{X}\to\mathop{\mathrm{Aut}}\nolimits(\mathcal{L}[X]) permitting us to think of ΣX\mathbb{Z}\ltimes\Sigma_{X} as a subgroup of the automorphism group.

We highlight two additional properties of ΣX\mathbb{Z}\ltimes\Sigma_{X}. It acts cocompactly on [X]\mathcal{L}[X] as any copy of XX gives a compact set whose translates cover [X]\mathcal{L}[X]. And, since any copy of XX can be mapped to any other copy of XX, the action of ΣX\mathbb{Z}\ltimes\Sigma_{X} on [X]\mathcal{L}[X] is essential. Next, we will show that ΣX\mathbb{Z}\ltimes\Sigma_{X} satisfies a law and thus, for nontrivial ΣX\Sigma_{X}, has finite girth.

Recall that a group Γ\Gamma satisfies a law if there is a word w(x1,x2,,xn)w(x_{1},x_{2},\ldots,x_{n}) on nn letters such that w(γ1,γ2,,γn)=1w(\gamma_{1},\gamma_{2},\ldots,\gamma_{n})=1 in Γ\Gamma for any γ1,γ2,,γnΓ\gamma_{1},\gamma_{2},\ldots,\gamma_{n}\in\Gamma. That ΣX\mathbb{Z}\ltimes\Sigma_{X} satisfies a law can be shown from observing that both ΣX\Sigma_{X} and ΣX/ΣX{\mathbb{Z}\ltimes\Sigma_{X}}/\Sigma_{X}\cong\mathbb{Z} satisfy a law. However, the space [X]\mathcal{L}[X] provides a geometric proof which we provide.

Lemma 18.

For a compact CAT(0)\operatorname{CAT(0)} cube complex XX which has diametrically opposed vertices, the group ΣX\mathbb{Z}\ltimes\Sigma_{X} satisfies a law.

Proof.

Let |Aut(X)|=n|\mathop{\mathrm{Aut}}\nolimits(X)|=n and x=(σ1,τk)x=(\sigma_{1},\tau^{k}) and y=(σ2,τl)y=(\sigma_{2},\tau^{l}) be elements in ΣX\mathbb{Z}\ltimes\Sigma_{X}. Note that the commutator [x,y][x,y] acting on [X]\mathcal{L}[X] maps each copy of XX to itself. Clearly then, [x,y]n[x,y]^{n} acts trivially. Since the action is faithful, [x,y]n[x,y]^{n} must then be the identity. ∎

Although a sketch of the proof for the following result can be found elsewhere in the literature (see Proposition 1 in [Dyu00]), we provide a proof for completeness.

Lemma 19.

If a group HH is not solvable, then H\oplus_{\mathbb{Z}}H is not virtually solvable.

Proof.

Let GHG\leq\oplus_{\mathbb{Z}}H be a finite index subgroup. We claim that, for some ii, the projection map πi:GH\pi_{i}:G\rightarrow H to the ithi^{th} factor is surjective. If not, then for each ii there is a nontrivial element aia_{i}, in the ithi^{th} factor, with aiπi(G)a_{i}\notin\pi_{i}(G). Consider the elements bi=(,e,ai,e,)b_{i}=(\ldots,e,a_{i},e,\ldots) in the direct sum, where aia_{i} appears in the ithi^{th} position. It follows that πi(bibj1)=ai\pi_{i}(b_{i}b_{j}^{-1})=a_{i} for iji\neq j, implying that bibj1Gb_{i}b_{j}^{-1}\notin G for all such i,ji,j. Then, biG=bjGb_{i}G=b_{j}G if and only if bi=bjb_{i}=b_{j}. Since bib_{i} is nontrivial for all ii\in\mathbb{Z}, GG has countably many distinct cosets and hence cannot be a finite index subgroup. Thus the map πi:GH\pi_{i}:G\rightarrow H is a surjection for some ii, and we conclude that a finite index subgroup GG of H\oplus_{\mathbb{Z}}H necessarily surjects onto HH. Since HH is non solvable, GG is non solvable. ∎

Now, consider the subgroup ΣXΣX\Sigma_{X}\leq\mathbb{Z}\ltimes\Sigma_{X}. By Lemma 19, if Autv,v(X)\mathop{\mathrm{Aut}}\nolimits_{v,v^{*}}(X) is not solvable then ΣX\Sigma_{X} is not virtually solvable, and hence neither is ΣX\mathbb{Z}\ltimes\Sigma_{X}. This fact combines with lemma 18 to give the following.

Example 20.

If Autv,v(X)\mathop{\mathrm{Aut}}\nolimits_{v,v^{*}}(X) is non-solvable then ΣX\mathbb{Z}\ltimes\Sigma_{X} provides an example of a group acting essentially and cocompactly on a finite dimensional CAT(0) cube complex that is not virtually solvable yet satisfies a law. Consequently, this example shows that the Girth Alternative, as stated in Corollary B, fails for the class of groups acting cocompactly on finite dimensional CAT(0) cube complexes.

As a special instance, for X=InX=I^{n}, Autv,v(X)Sn\mathop{\mathrm{Aut}}\nolimits_{v,v^{*}}(X)\cong S_{n}. Thus, for n5n\geq 5, ΣXSn\mathbb{Z}\ltimes\Sigma_{X}\cong S_{n}\wr\mathbb{Z} provides a more concrete example.

5. Questions and Remarks

  1. (1)

    Can we drop the lattice assumption in Theorem 10 and instead assume that Γ\Gamma acts essentially on XX?

    As suggested in Remark 15, an affirmative answer to the above question depends on an affirmative answer to the following question: Can we drop the ‘lattice’ assumption in Theorem 5 and instead assume that Γ\Gamma acts essentially on XX?

  2. (2)

    Remark 16 motivates us to ask the following question. Suppose X=X1×X2××XnX=X_{1}\times X_{2}\times\ldots\times X_{n} where XiX_{i} are irreducible and ΓAut(X)\Gamma\leq\mathop{\mathrm{Aut}}\nolimits(X). Let Γ\Gamma^{\prime} be the finite index subgroup of Γ\Gamma that stabilizes each irreducible factor XiX_{i}. If Girth(Γ)\operatorname{Girth}(\Gamma^{\prime}) is infinite, must Girth(Γ)\operatorname{Girth}(\Gamma) be infinite?

  3. (3)

    Can we generalize any of statements of theorem A through C to groups acting on non-locally compact cube complexes? This question is again motivated by the analogous Tits Alternatives of [CS11], where local compactness was not required.

  4. (4)

    Are the alternatives in Theorem 10 mutually exclusive? In other words, under the hypothesis of Theorem 10, if Γ\Gamma virtually fixes some point in XXX\cup\partial_{\infty}X, does that imply Girth(Γ)<\operatorname{Girth}(\Gamma)<\infty.

6. Acknowledgements.

We are very grateful to Azer Akhmedov for the valuable suggestions and comments on the initial draft of the paper. We are thankful to Pierre-Emmanuel Caprace for helpful conversations.

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