On the Girth of Groups Acting on CAT(0) Cube Complexes
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 with a fixed generating set , it makes sense to talk about the girth of it’s Cayley graph, denoted . Then, one can define the girth of the group as the supremum of the girth of the Cayley graphs over all finite generating sets of i.e.
Note that measures the length of the shortest non-trivial word relation in the Cayley graph . 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 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 of finitely generated groups, is said to satisfy the Girth Alternative if for any group , either is virtually solvable (and hence has finite girth unless isomorphic to ) or girth of 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 of finitely generated groups, is said to satisfy Tits Alternative if for any group , either is virtually solvable or contains a non-abelian free subgroup .
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 as a subgroup, see Theorem 5.3.E in [Gro87]), mapping class groups of compact surfaces ([Iva84], [BLM83]), Out() ([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 ([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 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() 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 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 be a product of irreducible, unbounded, and locally compact cube complexes such that acts cocompactly and essentially on for all .
Then for any (possibly non-uniform) lattice acting properly on , either is {locally finite}-by-{virtually abelian} or .
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 be a product of irreducible, unbounded, and locally compact cube complexes such that acts cocompactly and essentially on for all . Suppose is a lattice (possibly non-uniform) acting properly on and has a bound on the order of its finite subgroups.
Then is either virtually abelian or . In particular, 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 be a product of irreducible, unbounded, locally compact cube complexes such that acts cocompactly and essentially on for all .
Then for any (possibly non-uniform) lattice , either virtually fixes some point in or .
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 . We define an -cube, or simply cube, as the product (with ). A face of is the restriction of some number (possibly zero) of its coordinates to or , and a midcube of is the restriction of precisely one of its coordinates to . Cleary, midcubes of can be realized as -cubes and we will often treat them as such. We will refer to -cubes, -cubes, and -cubes as vertices, edges, and squares respectively.
A cube complex is a cell complex where the cells are -cubes, for various , and the attaching maps are Euclidean isometries in faces. We say the dimension of a cube complex is , or is finite dimensional, if contains -cubes but not -cubes, for some . If no such exists, we say that is infinite dimensional. is locally finite if every vertex of meets only finitely many cubes. In the setting of cube complexes, being locally finite is equivalent to being locally compact.
Two cube complexes and are isomorphic if there is a bijection between their vertex sets such that, if is an -cube in then is an -cube in . In particular, an isomorphism of cube complexes maps adjacent vertices to adjacent vertices.
A subcomplex of a cube complex is any collection of cubes in inheriting the same attaching maps. We will denote subcomplexes by . We call irreducible if there do not exist cube complexes with . Note that, if , then contains subcomplexes isomorphic to and . Cube complexes need not be connected.
A cube complex is a CAT(0) space if extending the Euclidean metric on individual cubes to the path length metric on 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 , will guarantee that is locally CAT(0). A finite dimensional cube complex is locally CAT(0) if the link of every vertex in is a simplicial flag complex. If, in addition, is simply-connected then being locally CAT(0) implies that 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 , the decomposition into irreducible factors is unique up to a permutation of its factors by the following proposition.
Proposition 1 ([CS11]).
A finite dimensional cube complex admits a canonical decomposition
into a product of irreducible cube complexes . Every automorphism of preserves that decomposition, up to a permutation of possibly isomorphic factors. In particular, the image of canonical embedding
has finite index in .
When it is necessary to treat as a metric space, we will use to denote the CAT(0) metric. With this metric, is a unique geodesic space.
2.2. Hyperplanes and Halfspaces
For a cube complex , we say two edges are related if and there is a square in containing and .
Informally, and are related if they are opposite edges of a square. A hyperplane in , typically denoted as , is the transitive closure of this relation on a single edge. The collection of all hyperplanes in a cube complex is denoted . For the geometric realization of a hyperplane, first observe that any nonempty collection of related edges in an -cube uniquely determine a midcube of . Midcubes in therefore inherit a relation from the edges. One then sees that two midcubes and are related whenever their intersection is a common face. The geometric realization of is the transitive closure of this relation on a single midcube. In this instance, midcubes and inherit attaching maps from their corresponding cubes.
For the remainder, we use the same symbol, , to denote both a hyperplane and its geometric realization.
Two hyperplanes and are transverse, denoted , if there is a square in containing edges and with , and . Note that if and only if their geometric realizations intersect. If and are not transverse, they are nested. We say and are separated if there is a third hyperplane containing and in complimentary halfspaces, and they are strongly separated if they are separated and there does not exist a hyperplane transverse to both and .
Properties of Hyperplanes. Let be a CAT(0) cube complex and
-
(1)
is a CAT(0) cube complex in its own right.
-
(2)
separates into two components.
Recent proofs of these properties can be found in [Far16]. We denote the closures of the two components of by and , which we also refer to as halfspaces. Choosing which component to call for all defines a labeling of . The collection of halfspaces of is denoted . A halfspace is deep if the distance from to points in is unbounded. Otherwise, is shallow. Halfspaces and are nested if either or . Note that if hyperplanes and are nested then they each have a halfspace which together form a nested pair. We also call and strongly separated if and are strongly separated.
2.3. Boundaries and Regular Points
The collection of halfspaces of a CAT(0) cube complex forms a poset with partial order given by set-inclusion, and comes naturally equipped a complimentary map given by the involution . Let denote the collection of ultrafilters of , that is, satisfies the two conditions
-
(1)
(Choice) for every pair , exactly one of them is in , and
-
(2)
(Consistency) if and with , then .
Given an ultrafilter , any subset is guaranteed to satisfy the so called partial choice condition: for every pair , at most one of them is in .
A nested sequence of halfspaces is called descending (or a descending chain) if for all . A descending sequence of halfspaces is terminating if , for some and all . Otherwise is nonterminating. Given , we say satisfies the descending chain condition (DCC) if every descending sequence in is terminating. Note that descending sequences necessarily satisfy the partial choice condition.
One has a bijective correspondence between the vertex set of and ultrafilters in satisfying the DCC given by , where . Given a vertex , choosing the halfspace containing to call for all hyperplanes gives a labeling of , which we refer to as being determined by .
Now, let . Then is compact in the Tychonoff topology and the choice condition induces an inclusion in which embeds as a closed subset which is therefore compact. We call the image of the Roller compactification and denote it by . To realize the image of in concretely, start by defining by
Then, the map with coordinate functions gives an embedding as a dense open subset. See [Rol16] and [NS13] for details. Note that the Roller compactification behaves well with respect to products. Indeed, if then . The Roller Boundary of , denoted , is the remainder space . It is a fact that agrees with the collection of ultrafilters in that do not satisfy the DCC. Note that an element necessarily contains a nonterminating descending sequence. Of paramount interest to us is the case that contains a nonterminating descending sequence of strongly separated halfspaces, . We call such a regular point. These were originally defined in [Fer18] (and independently in [KS16]) as elements such that if then there exists with and is strongly separated from both and . They were also shown to be equivalent to the definition provided. [FLM18, Proposition 5.13] and Lemma 8 below imply that, if is a regular point containing a nonterminating descending sequence of strongly separated halfspaces, , and if is a regular point with then . Due to this fact, we will often refer to a regular point, , simply as a nonterminating descending sequence of strongly separated halfspaces, .
The visual boundary of a CAT(0) cube complex 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 .
2.4. Groups Acting on Cube Complexes
An element is an automorphism if it acts as a cubical isomorphism of . We let denote the group of automorphisms of . A subgroup of in is said to act cocompactly if there exists a compact subcomplex whose translates cover , i.e., . Under our assumption that is locally compact, this is equivalent to requiring that be compact. acts essentially if given any halfspace in , we have is unbounded. Note that, for to act essentially, the halfspaces of must be deep.
For a CAT(0) cube complex, upon passing to its barycentric subdivision, elements come in two types ([Hag07]):
-
(1)
(Elliptic) fixes a vertex in ;
-
(2)
(Hyperbolic) is not elliptic and preserves a geodesic line.
A geodesic line preserved by is called an axis for . A rank one isometry is a hyperbolic automorphism none of whose axes bound a flat halfplane, and a contracting isometry is a rank one isometry with axis such that the diameter of the orthogonal projection to of any ball disjoint from is bounded above. An element in is regular if it acts as a contracting isometry on each irreducible factor of .
Contracting isometries can be detected by looking at their action on strongly separated hyperplanes. An element is said to double skewer the pair of hyperplanes if there is a nested pair of halfspaces of such that .
Lemma 2 ([CS11]).
Let be a finite dimensional cube complex and double skewers a pair of strongly separated hyperplanes in . Then is a contracting isometry.
Suppose double skewers . Then for some choice of halfspace of the hyperplane , and give us two nonterminating descending sequence of halfspaces. Moreover, if and are strongly separated hyperplanes, then both and are nonterminating descending sequences of strongly separated halfspaces, and hence correspond to two regular points in . In this case can be thought as acting along an axis whose end points are and . We refer to and as poles of .
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 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 be a group acting on a set . Suppose there exist elements , subsets , and a point , such that
-
(1)
-
(2)
for all
-
(3)
for all .
Then is non-abelian free subgroup of .
However, mere containment of a copy of 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 be a group acting on a set with a finite generating set . Suppose there exist elements , subsets , and a point such that
(1) | ||||
(2) | ||||
(3) |
Then is a non-cyclic group with .
Clearly, the elements and subsets in Theorem 4 satisfy the conditions in Proposition 3 and therefore 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 cube complexes, the role of such isometries are played by contracting isometries. In general, a finite dimensional 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 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 be a product of irreducible, unbounded, locally compact cube complexes such that acts cocompactly and essentially on for each . Suppose that is a lattice (possible non-uniform). Suppose that are nested halfspaces in each factor . Then there exists a regular element which simultaneously double skewers these hyperplanes. That is to say, for each , .
The above Theorem reduces the problem of finding a regular element in to finding a pair of strongly separated hyperplanes in each irreducible factor of . 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 , each containing two pairs of strongly separated hyperplanes, then the group elements that skewer the strongly separated pairs in each 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 will mean the set consisting of two elements and whereas the notation will stand for a sequence . 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 be an irreducible finite dimensional cube complex where acts essentially and without fixed points at infinity. Let be a facing triple in with and strongly separated. Then for any , there exists a collection of facing hyperplanes such that each pair is strongly separated for all .
An automorphism is said to flip a halfspace , if . 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 can be flipped under certain conditions.
Theorem 7 (Flipping Lemma [CS11]).
Let be finite dimensional cube complex and be a group acting essentially without a fixed point at infinity. Then for any halfspace , there is some such that .
Proof of Lemma 6.
It is convenient to prove the lemma in terms of the halfspaces. Suppose is the facing triple of halfspaces. Let and . We start by applying an automorphism to the pair that flips the halfspace to get the pair . Clearly the are facing halfspaces and the pair is strongly separated. By induction, suppose we have constructed the facing halfspaces such that and are strongly separated for each where . To construct facing hyperplanes, we apply an automorphism to the triple that flips to get and then apply another automorphism to the pair that flips to get another pair [See figure 1]. By construction, and are both pairs of strongly separated hyperplanes. Finally, we claim that the collection consists of facing halfspaces [Figure 1].
First, we observe that halfspaces in the collection are mutually disjoint. This is because and are contained in , and the pair is obtained by applying an automorphism to the pair that flips . It follows that both and are contained inside . The claim follows. Next we show that both and are disjoint from the collection . By construction, is obtained by applying an automorphism to the pair that flips , therefore both and are contained inside . Since is disjoint from any set from the collection , so are both and .
Similarly, we can show both and are disjoint from the collection . First note that, by construction. Also, and . Consequently both and are contained inside which is disjoint from any set from the collection . This finishes the proof. ∎
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 and are disjoint if for some . Otherwise, we say that and 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 and be two disjoint descending sequence of halfspaces in a finite dimensional cube complex . Let be another descending sequence of strongly separated halfspaces in that intersects . Then and are disjoint.
Proof.
We need to show that for sufficiently large . By hypothesis, there exist such that for all . Since is descending and intersects , there exists such that . So, either , or or .
Next, we will show how to rule out the second and third cases by taking large enough. To rule out the second case, we observe that for all . However, since is finite dimensional, there can be at most finitely many hyperplanes between any two halfspaces. So, for large enough , the second case does not occur. To rule out the third case, suppose for some . Since and are strongly separated, cannot be transverse to . So, either or . By hypothesis . Therefore, we have .
So we are left with the first possibility which is for some . Since , it follows that . Since the sequences of halfspaces are descending, we get is disjoint from . ∎
We say that a cube complex is -like if there is an -invariant geodesic line in . The final ingredient to our main theorem is the following Lemma which characterizes cube complexes with invariant Euclidean flats.
Lemma 9 ([CS11]).
Let be a finite dimensional cube complex such that acts essentially. Then stabilizes some -dimensional flat if and only if decomposes as a product of subcomplexes, each of which is essential and -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 be a product of irreducible, unbounded, locally compact cube complexes such that acts cocompactly and essentially on for all .
Then for any (possibly non-uniform) lattice , either virtually fixes some point in or .
Proof.
Suppose does not fix a point in . We want to show that .
Since does not have fixed points at infinity, does not have fixed points at infinity. Furthermore, since acts essentially on , we can invoke [CS11, Proposition 5.1] to obtain a pair of strongly separated hyperplane in each .
We now apply Theorem 5 to obtain an element that double skewers in each . Let be the halfspace corresponding to the hyperplane such that for any . Since are strongly separated hyperplanes, it follows that and are two disjoint descending sequence of strongly separated halfspaces. In other words, they are the poles of in (see preliminaries).
Next, we choose an arbitrary generating set of . We will consider the translate of poles of in each under this generating set. More precisely, we consider the following list of descending sequences of halfspaces:
() |
where and . Since isometries preserve strong separation, all the sequences in the above list consists of strongly separated halfspaces.
(Also note that, for a fix , all the halfspaces in the above list may not live in , because can switch isomorphic factors. However, they all live in some ).
Now, we are going to produce another regular element such that the poles in each are disjoint from the list ( ‣ 3). In particular, its poles will be disjoint from that of . This is where we are going to use the fact that does not fix a point in . This will ensure that each is large, in a certain sense. More precisely, we will see that each has a facing triple.
First we observe that, since each is finite dimensional and locally compact and acts essentially and cocompactly on , by [CS11, Theorem 7.2], either stabilizes some Euclidean flat or there is a facing triple of hyperplanes in .
Suppose stabilizes some Euclidean flat . Since is irreducible, it follows from Lemma 9 that is R-like. Thus has an index two subgroup which fixes a point at infinity contradicting our assumption on . Therefore, we have a facing triple of hyperplanes in each . 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 that are facing each other. Given a pair of strongly separated hyperplanes taken from each , we can choose an element from that double skewers each pair in the corresponding 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 . Of these infinitely many descending sequences of halfspaces in , all but finitely many are disjoint from the list ( ‣ 3) by Lemma 8 because the list ( ‣ 3) contains a finite number of descending sequences of strongly separated halfspaces. In particular, there exists a pair of disjoint halfspaces in each , such that for large enough , both and are disjoint from the following collection
Let be an element that double skewers in each . Without loss of generality, let us assume that and are the poles of in .
We let . Note that acts on . We set and .
Note that, the complement of in get sent to under high enough power of . Taking union over , we obtain that complement of in get sent to under high enough power of . Similarly, complement of in get sent to under high enough power of . We set , , where we choose so large that for all , we have
() |
Next, we observe that, by construction, and its translates under the generating set and their inverses do not intersect . In other words we have,
() |
Since iff for any , it follows from () that and its translates under the generating set and their inverses do not intersect . In other words, we have
() |
Furthermore, we can assume (by taking large enough) that the following set
is nonempty and for convenience, let us call this set .
We claim that , and any point satisfies the three properties of Lemma 4.
The first property is immediate by our choice of . To check the second property, note that and together with () this implies
which is the desired second property.
Therefore, 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 be a product of irreducible, unbounded, and locally compact cube complexes such that acts cocompactly and essentially on for all .
Then for any (possibly non-uniform) lattice acting properly on , either is {locally finite}-by-{virtually abelian} or .
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 .
Lemma 12.
Suppose acts by automorphism on a locally finite cube complex . Suppose be a -invariant subset and does not fix point-wise. Then there exists such that
Proof.
By the assumption, we can choose such that for some . Now we have two cases to consider.
Suppose is a vertex in . Since acts by automorphisms, translates of can only be other vertices. It follows that is at least the minimum of the distances between and other vertices. Since is locally finite, it follows that .
If is not a vertex, then is in the interior of some cube in . The infimum of distances between and all the translates of that are inside a different cube is clearly positive. Since there are only finitely many automophisms of , there are only finitely many nontrivial translates of that stay inside . Therefore the minimum distance from to any of its translates inside is also positive. The claim follows. ∎
Lemma 13.
Suppose acts on by isometries such that for some
Then there exists a finite index subgroup of and an -equivariant triangulation of .
Proof.
Let be the index two subgroup of consisting of only the orientation preserving isometries. In particular, acts by translation on and hence is a subgroup of . Either is trivial or implies that
It follows that is generated by the isometry that translates by amount. Therefore, placing the vertices at integer multiples of , we obtain a -equivariant triangulation of . ∎
Combining the above two lemmas we immediately get the following.
Lemma 14.
Suppose acts by automorphisms on a locally finite -like cube complex and let be an -invariant bi-infinite geodesic in . Then there exists a finite index subgroup of and a -equivariant triangulation of .
Proof.
Proof of Theorem 11.
It follows from [CL10, Theorem 1.7] that is {locally finite}-by-{virtually abelian} if and only if is amenable. Thus it is enough to show that if is not amenable, then . Suppose is non-amenable. We claim there is an irreducible factor of that is not -like.
If each irreducible factor of is -like, then we can take the -invariant geodesic in each factor and take their product to get an invariant -dimensional Euclidean flat. Let be the finite index subgroup of that stabilizes each factor. In particular, stabilizes the bi-infinite geodesic lines in each factor. Applying Lemma 14 to the action of on each -like factor, we get a finite index subgroup of which acts by automorphisms on some triangulation of the bi-infinite geodesic line in that -like factor. Taking the intersection of all these finite index subgroup for each factor we get another finite index subgroup that acts by automorphisms on each triangulated geodesic line. therefore acts by automorphisms on a Euclidean flat where is the product of triangulated geodesic lines. By [Gen22, Lemma 2.8], the set of bounded components in the Roller boundary of is finite and nonempty. These bounded components have cubical structure that is respected by the induced action of . Furthermore, the action of stabilizes the union of these bounded components. In particular, stabilizes some finite set of vertices in the Roller boundary and consequently a finite index subgroup of fixes a point in the Roller boundary of . By [CL11, Theorem A.5], is amenable. Since is a finite index subgroup, is amenable. This is a contradiction.
Hence at least one irreducible factor of is not -like, and hence contains a facing triple by [CS11, Theorem 7.2]. Now, we can discard all the -like factors from to get a space such that each irreducible factor of has a facing triple. Now we can run the same argument as in Theorem 10 to conclude that the girth of is infinite. ∎
Remark 15.
In our Girth Alternative theorems, we require the group to be a lattice in 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 . 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 has a finite index subgroup 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 -action on to prove that either virtually fixes a point or without assuming to be lattice: since we can forget about the other factors, we only need and to act as contracting isometries on , 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 implies . 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 , we call a pair of vertices diametrically opposed if there exists a labeling of the halfspaces of so that and . Note that a CAT(0) cube complex contains diametrically opposed vertices if and only if there is a geodesic path between vertices that crosses every hyperplane in .
If and are CAT(0) cube complexes each containing a pair of diametrically opposed vertices, then their product will contain a pair of diametrically opposed vertices. Indeed, if and define vertices , and and define vertices , then and give diametrically opposed vertices in .
Definition 17 (Cube Complex ).
Begin with a CAT(0) cube complex which contains diametrically opposed vertices and . For all , let be an isomorphic copy of , where and denote the images of and , respectively. The cube complex is then formed by identifying with for all . We think of informally as a “line of ’s.”
The space is clearly a cube complex as the map attaching distinct copies of is an isometry of . That is locally CAT(0) is also clear, since the link of a vertex labeled (or ) in is isomorphic to the disjoint union of two copies of the link of in . Lastly, is simply-connected by construction.
There is a natural action of on whereby each copy is shifted to an adjacent copy. With denoting the automorpisms fixing both and , acts on by allowing only finitely many coordinate groups to act nontrivially at a time. Clearly is the identity element. We are interested in the semi-direct product , where multiplication is defined as and . Note that is generated by the group and a single shift.
We define a group action of on by
This action is faithful since acts trivially if and only if both and are the identity element in and , respectively. Since it acts faithfully, there is an injective map permitting us to think of as a subgroup of the automorphism group.
We highlight two additional properties of . It acts cocompactly on as any copy of gives a compact set whose translates cover . And, since any copy of can be mapped to any other copy of , the action of on is essential. Next, we will show that satisfies a law and thus, for nontrivial , has finite girth.
Recall that a group satisfies a law if there is a word on letters such that in for any . That satisfies a law can be shown from observing that both and satisfy a law. However, the space provides a geometric proof which we provide.
Lemma 18.
For a compact cube complex which has diametrically opposed vertices, the group satisfies a law.
Proof.
Let and and be elements in . Note that the commutator acting on maps each copy of to itself. Clearly then, acts trivially. Since the action is faithful, 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 is not solvable, then is not virtually solvable.
Proof.
Let be a finite index subgroup. We claim that, for some , the projection map to the factor is surjective. If not, then for each there is a nontrivial element , in the factor, with . Consider the elements in the direct sum, where appears in the position. It follows that for , implying that for all such . Then, if and only if . Since is nontrivial for all , has countably many distinct cosets and hence cannot be a finite index subgroup. Thus the map is a surjection for some , and we conclude that a finite index subgroup of necessarily surjects onto . Since is non solvable, is non solvable. ∎
Now, consider the subgroup . By Lemma 19, if is not solvable then is not virtually solvable, and hence neither is . This fact combines with lemma 18 to give the following.
Example 20.
If is non-solvable then 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 , . Thus, for , provides a more concrete example.
5. Questions and Remarks
-
(1)
Can we drop the lattice assumption in Theorem 10 and instead assume that acts essentially on ?
-
(2)
Remark 16 motivates us to ask the following question. Suppose where are irreducible and . Let be the finite index subgroup of that stabilizes each irreducible factor . If is infinite, must be infinite?
- (3)
- (4)
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.
References
- [Akh03] Azer Akhmedov “On the girth of finitely generated groups” In Journal of Algebra 268, 2003, pp. 198–208
- [Akh05] Azer Akhmedov “The girth of groups satisfying Tits Alternative” In Journal of Algebra 287.2, 2005, pp. 275–282
- [Akh24] Azer Akhmedov “Girth Alternative for subgroups of ” In Glasgow Mathematical Journal, 2024, pp. 1–10
- [AM23] Azer Akhmedov and Pratyush Mishra “Girth Alternative for HNN extensions” In arXiv e-prints, 2023, pp. arXiv:2211.13326v3
- [BFH97] Mladen Bestvina, Mark Feighn and Michael Handel “The Tits alternative for Out() I: Dynamics of exponentially-growing automorphisms” In Annals of Mathematics 151, 1997, pp. 517–623
- [BFH97a] Mladen Bestvina, Mark Feighn and Michael Handel “The Tits alternative for Out() II: A Kolchin type theorem” In Annals of Mathematics 161, 1997, pp. 1–59
- [Ble05] Collin Bleak “Solvability in groups of piecewise-linear homeomorphisms of the unit interval” Thesis (Ph.D.)–State University of New York at Binghamton ProQuest LLC, Ann Arbor, MI, 2005, pp. 111
- [BLM83] Joan S. Birman, Alex Lubotzky and John McCarthy “Abelian and solvable subgroups of the mapping class groups” In Duke Mathematical Journal 50.4, 1983, pp. 1107–1120
- [BS85] Matthew G. Brin and Craig C. Squier “Groups of piecewise linear homeomorphisms of the real line” In Invent. Math. 79.3, 1985, pp. 485–498
- [CL10] Pierre-Emmanuel Caprace and Alexander Lytchak “At infinity of finite-dimensional CAT(0) spaces” In Math. Ann. 346.1, 2010, pp. 1–21
- [CL11] Pierre-Emmanuel Caprace and Jean Lécureux “Combinatorial and group-theoretic compactifications of buildings” In Ann. Inst. Fourier (Grenoble) 61.2, 2011, pp. 619–672
- [CM07] Yves Cornulier and Avinoam Mann “Some Residually Finite Groups Satisfying Laws” In Geometric Group Theory Basel: Birkhäuser Basel, 2007, pp. 45–50
- [CS11] Pierre-Emmanuel Caprace and Michah Sageev “Rank Rigidity for Cat(0) Cube Complexes” In Geometric and Functional Analysis 21.4, 2011, pp. 851–891
- [Dyu00] Anna Dyubina “Instability of the virtual solvability and the property of being virtually torsion-free for quasi-isometric groups” In International Mathematics Research Notices 2000.21, 2000, pp. 1097–1101
- [Far16] Daniel Farley “A Proof of Sageev’s Theorem on Hyperplanes in CAT(0) Cubical Complexes” In Topology and Geometric Group Theory Cham: Springer International Publishing, 2016, pp. 127–142
- [Fer18] Talia Fernós “The Furstenberg–Poisson boundary and CAT(0) cube complexes” In Ergodic Theory and Dynamical Systems 38.6, 2018, pp. 2180–2223
- [FLM18] Talia Fernós, Jean Lécureux and Frédéric Mathéus “Random walks and boundaries of cubical complexes” In Comment. Math. Helv. 93.2, 2018, pp. 291–333
- [Gen22] Anthony Genevois “Median Sets of Isometries in Cube Complexes and Some Applications” In Michigan Mathematical Journal 71.3, 2022, pp. 487–532
- [Gro87] M. Gromov “Hyperbolic Groups” In Essays in Group Theory 8, MSRI Publications Springer, New York, 1987, pp. 75–263
- [Hag07] Frédéric Haglund “Isometries of CAT(0) cube complexes are semi-simple” In Annales mathématiques du Québec 47, 2007, pp. 249–261
- [Iva84] N.. Ivanov “Algebraic properties of the Teichmüller modular group” In Dokl. Akad. Nauk SSSR 275.4, 1984, pp. 786–789
- [KS16] Aditi Kar and Michah Sageev “Ping pong on cube complexes” In Comment. Math. Helv. 91.3, 2016, pp. 543–561
- [Lea13] Ian J. Leary “A metric Kan–Thurston theorem” In Journal of Topology 6.1, 2013, pp. 251–284
- [Nak08] K. Nakamura “Some Results in Topology and Group Theory” University of California, Davis, 2008
- [Nak14] Kei Nakamura “The girth alternative for mapping class groups” In Groups Geom. Dyn. 8.1, 2014, pp. 225–244
- [NS13] Amos Nevo and Michah Sageev “The Poisson boundary of CAT (0) cube complex groups” In Groups, Geometry, and Dynamics 7.3, 2013, pp. 653–695
- [Rol16] Martin A. Roller “Poc Sets, Median Algebras and Group Actions” In arXiv: General Topology, 2016
- [Sch01] Saul Schleimer “On The Girth Of Groups”, 2001, pp. preprint
- [SW05] Michah Sageev and Daniel T. Wise “The Tits Alternative for Cat(0) Cubical Complexes” In Bulletin of the London Mathematical Society 37.5, 2005, pp. 706–710
- [Tit72] Jacques Tits “Free subgroups in linear groups” In Journal of Algebra 20, 1972, pp. 250–270
- [Yam11] Saeko Yamagata “The girth of convergence groups and mapping class groups” In Osaka Journal of Mathematics 48.1 Osaka UniversityOsaka Metropolitan University, Departments of Mathematics, 2011, pp. 233–249