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Le Conte de la Mesure sur les Complexes Cubiques CAT(0)

Talia Fernós Department of Mathematics, University of North Carolina, Greensboro dr.talia.fernos@gmail.com In honor of Mike Mihalik’s 70th birthday, happy birthday!
(Date: March 10, 2024)
Abstract.

We revisit the topic of probability measures on CAT(0) cube complexes and prove that an amenable group acting on a CAT(0) cube complex, regardless of dimension, necessarily preserves an interval in the Roller compactification. In the finite dimensional case, we prove that there must be an orbit of cardinality 2N2^{N}, where NN is bounded by the dimension. This is a slight extension of the author’s previuos Tits’ Alternative.

Key words and phrases:
CAT(0), Cube Complexes, Tits’ Alternative
2020 Mathematics Subject Classification:
Primary 54C40, 14E20; Secondary 46E25, 20C20
2020 Mathematics Subject Classification:
Primary 20F65, 20E05, 60B05; Secondary 05C12, 05E18, 06A07, 20F29
The author was partially supported by NSF grant DMS–2005640.
[Uncaptioned image]
\specialsection

Introduction The idea for this short paper came through preparations for a talk I gave in summer of 2023 at the Séminaire Virtuel Francophone – Groupes et Géométrie. The seminar is aimed to be expository in nature and so I thought I would revisit the topic of probability measures on CAT(0) cube complexes, and their associated intervals (see Section 0.6). This association was introduced by Monod and Shalom in [MS04, Proposition 4.5] for trees and developed further in my joint work with Chatterji and Iozzi [CFI16]. It was also used either implicitly or explicitly in [Fer18, FLM18, FLM21], and even [FFH23]. The key tool for this is the Lifting Decomposition which is discussed in Section Lemma.

As I was preparing my lecture, I realized that I could in fact make a small improvement on my previous contribution to the story of Tits’ Alternatives. Therefore, I take the opportunity to share that here. I also include some of the drawings I made (using notability on an ipad).

Theorem.

Let XX be a CAT(0) cube complex of finite dimension DD, and suppose that ΓAutX\Gamma\to\text{Aut}\,X preserves an interval in the Roller compactification X¯\overline{X}. Then Γ\Gamma must have an orbit in X¯\overline{X} of cardinality 2N2^{N}, for some 0ND0\leqslant N\leqslant D.

If XX is not finite dimensional and Γ\Gamma is assumed to be amenable then it must preserve an interval X¯\mathcal{I}\subset\overline{X}.

Combining with the Tits’ Alternative from [Fer18], we obtain the following (the reader should compare statements):

Corollary (Tits’ Alternative).

Suppose XX is a finite dimensional CAT(0) cube complex. Given a group action ΓAutX\Gamma\to\text{Aut}\,X either Γ\Gamma contains a freely acting free group on 2 generators, or Γ\Gamma has an orbit of cardinality 2N2^{N} in X¯\overline{X}, for some 0ND0\leqslant N\leqslant D, where DD is the dimension of XX.

Examples: The following examples show that the bounds above are optimal. We note that all the groups are amenable.

  • Consider the standard action of the infinite dihedral group D\mathrm{D}_{\infty} on \mathbb{Z}. Of course, there is no fixed point but there is an orbit of cardinality 2 in the Roller compactification, namely {±}\{\pm\infty\}.

  • Similarly, DN\mathrm{D}_{\infty}^{N} acts on N\mathbb{Z}^{N} and has a unique finite orbit which has cardinality 2N2^{N}.

  • Finally, nD\underset{n\in\mathbb{N}}{\overset{}{\oplus}}\mathrm{D}_{\infty} acts on n\underset{n\in\mathbb{N}}{\overset{}{\oplus}}\mathbb{Z} which is of course infinite dimensional, and does not have a finite orbit in the Roller compactification, but it is an interval.

We note that there are many Tits’ Alternatives available in the literature [Tit72, BFH04, SW05, CS11, Fio18, MP22, OP22, GJN23, Gen21]. However, in this brief note, I will not endeavor to give a comprehensive overview of the Tits’ Alternatives, nor to give a thorough account of CAT(0) cube complexes. The reader can see the references provided for further details.

Acknowledements: I thank Dafne Sanchez for help with the coloring scheme, inspired by Matisse. I also thank Indira Chatterji, François Dahmani, Anne Lonjou, and Yves Stalder for the invitation to speak at the Séminaire Virtuel Francophone – Groupes et Géométrie which inspired me to write this article. I thank all of my collaborators and mentors with whom I have discussed CAT(0) cube complexes for helping me explore how to understand and communicate their beauty. Finally, I thank the National Science Foundation for their generous support of my work, particularly through NSF grant DMS–2005640. \specialsectionBasics

A cube complex is a space obtained by gluing unit cubes isometrically along their faces. Moreover, it is said to be CAT(0) if it is nonpositively curved and simply connected.

You may think of the process of creating a CAT(0) cube complex as gluing together cubes in a particular order. If at some point there is positive curvature that is created locally, it is due to something as in Figure 1. There, we have created part of the boundary of a 3-dimensional cube by gluing 3 unit squares together. That creates a cone angle of 3π/23\pi/2. Since 3π/2<2π3\pi/2<2\pi, it is positively curved. However, we may annul the positive curvature by “filling” in the other side to create a 3-dimensional cube. Nonpositive curvature of a CAT(0) cube complex is equivalent to the Gromov Link Condition. We refer the reader to [Sag95, CN05, Nic04, Rol16] for more details.

Refer to caption
Figure 1. Making a cube complex CAT(0)

0.1. Functoriality: Walled Spaces

A useful way to think of CAT(0) cube complexes is via this functorial construction. Begin with a set YY together with a collection of (nonempty) two-sided (walls) partitions 𝒫2Y\mathcal{P}\subset 2^{Y}. Two sided here means that if h𝒫h\in\mathcal{P} then Yh𝒫Y\setminus h\in\mathcal{P}. The wall may be thought of as the pair {h,Yh}\{h,Y\setminus h\}.

Next, create a graph by declaring that each maximal non-empty intersection of sets from 𝒫\mathcal{P} is a vertex. We connect two vertices if their corresponding defining intersections differ by the choice of exactly one side of one partition from 𝒫\mathcal{P}. In Figure 2, you can see a choice of 5 partitions. Each region is not empty. The regions labeled AA and U1U_{1} differ by the choice of one partition and therefore, their associated vertices aa and u1u_{1} respectively are connected by an edge.

Refer to caption
Figure 2. Functorial Construction

Once we have done this, we may not have a CAT(0) cube complex. However, we may take the cubical completion (as in Figure 2, where we must add the unlabled “back” vertex to creat a 3-cube) to annul positive curvature. We note that this can always be done, except that distances may become infinite (if there are infinitely many partitions separating two regions, i.e. the finite interval condition is not satisfied) or the dimension may become infinite (if there are families of pairwise transverse partitions of unbounded cardinality, see Section 0.3 for the definition of transverse).

Conversely, start with (the vertex set of) a CAT(0) cube complex XX. Each edge in XX belongs to an equivalence class generated by “being parallel across a square”. The compliment of that parallelism class has two sides, and the vertices that belong to each side give the two-sided partition of the vertex set (see Figure 3).

Finally, if we apply the previous construction to this collection of two-sided partitions, we get a CAT(0) cube complex, which is cannonically isomorphic to (the vertex set of) XX.

Refer to caption
Figure 3. Two CAT(0) Cube Complexes with 10 halfspaces

0.2. The Roller Compactification

A halfspace of a CAT(0) cube complex is one side of a two-sided partition, as discussed above. We have established that the vertex set, denoted by XX, is cannonically determined by the halfspace structure 2X\mathfrak{H}\subset 2^{X}. By mapping a vertex in XX to the collection of halfspaces that contain it, we obtain an isometric injection:

X2.X\hookrightarrow 2^{\mathfrak{H}}.

Here the extended metric on 22^{\mathfrak{H}} is given by half the cardinality of the symmetric difference d(S,T)=12(ST)[0,]d(S,T)=\frac{1}{2}(S\triangle T)\in[0,\infty]. While this metric is useful, we will rely on the standard topology on 2Map({0,1})2^{\mathfrak{H}}\cong\mathrm{Map}(\mathfrak{H}\to\{0,1\}). This is given by declaring the basic open sets to be cylinder sets, which are themeselves determined by specifying values in finitely many coordinates. Equivalently, this is the topology of pointwise convergence of maps {0,1}\mathfrak{H}\to\{0,1\}. With this topology, 22^{\mathfrak{H}} is compact. We note that the induced topology may be different than the metric topology on XX. This is directly comparable to the weak-* topology and respectively the metric topology on a Hilbert space.

Having found an injection of XX into the compact space 22^{\mathfrak{H}}, we may take the closure in the image and this defines the Roller compactification. By removing the image of XX inside this closure, we are left with the Roller boundary.

Note that once we obtain the closure of XX in 22^{\mathfrak{H}}, there is a cannonical extension of the halfspaces as partitions of XX to X¯\overline{X}. Those are the basic clopen sets for our totally disconnected topology on X¯\overline{X}.

The following is then immediate from the functorial construction, and can be thought of as forgetfulness.

Corollary.

Let XX be a CAT(0) cube complex with halfspace structure \mathfrak{H}. Let \mathfrak{H}^{\prime}\subset\mathfrak{H} be involution invariant and XX^{\prime} the associated CAT(0) cube complex. Then the map 222^{\mathfrak{H}}\twoheadrightarrow 2^{\mathfrak{H}^{\prime}}, given by SSS\mapsto S\cap\mathfrak{H}^{\prime} induces a 1-Lipschitz projection X¯X¯\overline{X}\twoheadrightarrow\overline{X^{\prime}}.

We shall see in Section Lemma how and when we can find a cannonical section to this map. The example in Figure 4 is given by taking =\mathfrak{H}^{\prime}=\mathfrak{H}\setminus\mathcal{B} and a valence consideration shows that an isometric section is impossible.

Refer to caption
Figure 4. An example where a section to the projection is impossible

The Roller boundary of a tree is, as a set, the visual boundary, but the topology is different when it is not (large-scale) locally finite. Consider the tree given by identifying at 0 infinitely many copies of [0,][0,\infty], as in Figure 5. It is not difficult to see that n0\infty_{n}\to 0 since all halfspaces eventually contain 0.

The Roller compactification has an important multiplicative property:

X1×X2¯=X¯1×X¯2.\overline{X_{1}\times X_{2}}=\overline{X}_{1}\times\overline{X}_{2}.
Refer to caption
Figure 5. Halfspaces containing n\infty_{n}.

Refer to caption
Figure 6. The Roller Compactification for 2\mathbb{Z}^{2}

Refer to caption
Figure 7. Roller Compactification for F2×F_{2}\times\mathbb{Z}

Combining this, with the discussion for trees, we obtain the Roller compactification of 2\mathbb{Z}^{2}, as in Figure 6, or for F2×F_{2}\times\mathbb{Z} as in Figure 7.

0.3. Comparing halfspaces

Given a pair of halfspaces h,kh,k\in\mathfrak{H} such that kh,hk\neq h,h^{*} then either all of the pairwise intersections hk,hk,hk,hkh\cap k,h\cap k^{*},h^{*}\cap k,h^{*}\cap k^{*} are not empty (and in this case, we say that hh and kk are transverse, and write hkh\pitchfork k) or one of the following other cases hold (see Figure 8):

kh\displaystyle k\subset h\quad\,\, hk\displaystyle\quad\,\,h\subset k
hk=\displaystyle h^{*}\cap k^{*}=\varnothing hk=.\displaystyle h\cap k=\varnothing.
Refer to caption
Figure 8. The possible relationships between halfspaces h,kh,k, with kh,hk\neq h,h^{*}.
Lemma.

The dimension of XX is the supremum cardinality of subsets SS\subset\mathfrak{H} of pairwise transverse halfspaces.

It is straightforward to verify that if =12\mathfrak{H}=\mathfrak{H}_{1}\sqcup\mathfrak{H}_{2} is a nontrivial disjoint decomposition into nonempty involution invariant, pairwise transverse sets and XX, X1X_{1}, and X2X_{2} are the assocaited CAT(0) cube complexes respectively then there is a cannonical isomorphism XX1×X2X\cong X_{1}\times X_{2}. We say that XX is irreducible if it is not isomorphic to a product.

Theorem.

[CS11, Proposition 2.6] Let XX be finite dimensional. Then, there is a cannonical decomposition of XX into a product of irreducible CAT(0) cube complexes.

A pair of halfspaces h,kh,k\in\mathfrak{H}, with hkh\neq k^{*} are said to be facing if hk=h^{*}\cap k^{*}=\varnothing. This corresponds to the lower right corner in Figure 8. A triple of halfspaces h,k,h,k,\ell\in\mathfrak{H} are said to be a facing triple if they are pairwise facing.

0.4. Intervals in X¯\overline{X}

Let X¯\mathcal{I}\subset\overline{X} be an arbitrary subset. The (involution invariant) collection of halfspaces that separate points in \mathcal{I} is

:={h:h,h}.\mathfrak{H}_{\mathcal{I}}:=\{h\in\mathfrak{H}:h\cap\mathcal{I},h^{*}\cap\mathcal{I}\neq\varnothing\}.

Similarly, we denote the collection of halfspaces that contain \mathcal{I} as +\mathfrak{H}_{\mathcal{I}}^{+}, and the collection of compliments of halfspaces that contain \mathcal{I}, namely the halfspaces that trivially intersect \mathcal{I} is denoted by \mathfrak{H}_{\mathcal{I}}^{-}, meaning that =(+)\mathfrak{H}_{\mathcal{I}}^{-}=(\mathfrak{H}_{\mathcal{I}}^{+})^{*}. We have established the following decomposition:

=+.\mathfrak{H}=\mathfrak{H}_{\mathcal{I}}\sqcup\mathfrak{H}_{\mathcal{I}}^{+}\sqcup\mathfrak{H}_{\mathcal{I}}^{-}.

We say that, \mathcal{I} is an interval if there exists x,yX¯x,y\in\overline{X} such that =h{x,y}+h\mathcal{I}=\underset{h\in\mathfrak{H}_{\{x,y\}}^{+}}{\overset{}{\cap}}h. In this case we write =(x,y)\mathcal{I}=\mathcal{I}(x,y) and say that it is the interval between xx and yy. We also call xx and yy endpoints of \mathcal{I}. Clearly, (x,y)\mathfrak{H}_{\mathcal{I}(x,y)} does not contain a facing triple.

The structure of intervals in an arbitrary CAT(0) cube complex can be quite exotic; please see the examples in Figures 9 and 10 or come up with your own!

Nevertheless, the following theorem of [BCG+09], which relies on Dilworth’s Theorem for partially ordered sets, shows that intervals are not too wild.

Theorem.

Let DD be the dimension of XX. If X¯\mathcal{I}\subset\overline{X} is an interval then there exists an isometric embedding D¯\mathcal{I}\hookrightarrow\overline{\mathbb{Z}^{D}}.

Corollary.

If X¯\mathcal{I}\subset\overline{X} is an interval then the set of end points of \mathcal{I} has cardinality 2N2^{N}, for some 0ND0\leqslant N\leqslant D.

Refer to caption
Figure 9. The shaded region is an interval in the ambient CAT(0) cube complex
Refer to caption
Figure 10. This Roller compactification is an interval

0.5. The Helly Property in X¯\overline{X}

The following is an important property of halfspaces in a CAT(0) cube complex. The first item is the standard Helly property for halfspaces. The second follows from the first by applying the finite intersection property to the collection of sets 𝒮\mathcal{S}, each of which is clopen in the compact space X¯\overline{X}. Comparing it with the classical Helly property for convex sets in euclidean space, we may consider it as telling us that, in a sense, CAT(0) cube complexes are of Helly-dimension 1.

Lemma.

Suppose that 𝒮\mathcal{S}\subset\mathfrak{H} is such that hkh\cap k\neq\varnothing for all h,k𝒮h,k\in\mathcal{S}.

  • If #𝒮<\#\mathcal{S}<\infty then h𝒮hX\underset{h\in\mathcal{S}}{\overset{}{\cap}}h\cap X\neq\varnothing.

  • Otherwise X¯h𝒮h.\overline{X}\supseteq\underset{h\in\mathcal{S}}{\overset{}{\cap}}h\neq\varnothing.

\specialsection

Lifting Decompositions

Let XX be a CAT(0) cube complex with associated halfspace structure \mathfrak{H}. We shall say 𝒮\mathcal{S}\subset\mathfrak{H} is consistent if it satisfies the following two properties:

  1. (1)

    If h𝒮h\in\mathcal{S} then h𝒮h^{*}\notin\mathcal{S}.

  2. (2)

    If h,kh,k\in\mathfrak{H}, with hkh\subset k, and h𝒮h\in\mathcal{S} then k𝒮k\in\mathcal{S}.

We note that, according to the functorial construction, if 𝒮\mathcal{S} is consistent and 𝒮𝒮=\mathcal{S}\sqcup\mathcal{S}^{*}=\mathfrak{H} then 𝒮\mathcal{S} is the collection of halfspaces containing a single point.

Proposition.

Let XX be a CAT(0) cube complex with associated halfspaces \mathfrak{H} and 𝒮\mathcal{S}\subset\mathfrak{H} consistent. Set 𝒮:=(𝒮𝒮)\mathfrak{H}_{\mathcal{S}}:=\mathfrak{H}\setminus(\mathcal{S}\sqcup\mathcal{S}^{*}) and let X(𝒮)X(\mathfrak{H}_{\mathcal{S}}) be the associated CAT(0) cube complex. Then the map 2𝒮22^{\mathfrak{H}_{\mathcal{S}}}\to 2^{\mathfrak{H}} given by EE𝒮E\mapsto E\sqcup\mathcal{S} induces an isometric injection X¯(𝒮)X¯\overline{X}(\mathfrak{H}_{\mathcal{S}})\hookrightarrow\overline{X}, whose image is exactly

h𝒮hX¯.\underset{h\in\mathcal{S}}{\overset{}{\cap}}\,h\subset\overline{X}.

Furthermore, if 𝒮\mathcal{S} is Γ\Gamma-invariant, for some action ΓAut(X)\Gamma\to\text{Aut}\,(X) then with the restricted action on the image, the above natural injection is Γ\Gamma-equivariant.

0.6. Probability Measures

Consider a probability measure μProb(X¯)\mu\in\textrm{Prob}(\overline{X}) and the associated collection of halfspaces μ+:={h:μ(h)>1/2}\mathfrak{H}_{\mu}^{+}:=\{h\in\mathfrak{H}:\mu(h)>1/2\}. It is straightforward to verify that μ+\mathfrak{H}_{\mu}^{+} is consistent and that the collection of halfspaces μ={h:μ(h)=1/2}\mathfrak{H}_{\mu}=\{h\in\mathfrak{H}:\mu(h)=1/2\} does not contain any facing triples. Applying the Lifting Decomposition to μ+\mathfrak{H}_{\mu}^{+}, we get that hμ+h\underset{h\in\mathfrak{H}^{+}_{\mu}}{\overset{}{\cap}}\,h is isomorphic to X¯(μ)\overline{X}(\mathfrak{H}_{\mu}).

Lemma.

[CFI16, Lemma 4.7] If μProb(X¯)\mu\in\textrm{Prob}(\overline{X}) then X¯(μ)\overline{X}(\mathfrak{H}_{\mu}) is an interval.

0.7. Medians

Let x,y,zX¯x,y,z\in\overline{X} and consider the associated probability measure μ(x,y,z)=13(δx+δy+δz)\mu_{(x,y,z)}=\frac{1}{3}(\delta_{x}+\delta_{y}+\delta_{z}). A simple parity argument shows that if hh\in\mathfrak{H} then μ(x,y,z)(h)12\mu_{(x,y,z)}(h)\neq\frac{1}{2}. Therefore, we have that hμ+h\underset{h\in\mathfrak{H}_{\mu}^{+}}{\overset{}{\cap}}h is a single point, which we shall call the median of the triple and denote it by m(x,y,z)m(x,y,z).

While this is not the standard definition of the median, it fits nicely within our context. We note that several of the natural properties of the median (e.g. invariance under permutation of the points) are immediate, including the property that

m(x,x,y)=x.m(x,x,y)=x.
\specialsection

Proof of the Main Theorem

Suppose Γ\Gamma is amenable acting on XX. Since X¯\overline{X} is compact and metrizable, there must be a Γ\Gamma-invariant probability measure μProb(X¯)\mu\in\textrm{Prob}(\overline{X}). By the Lifting Decomposition and the previous lemma, it follows that hμ+h\underset{h\in\mathfrak{H}_{\mu}^{+}}{\overset{\,}{\cap}}h is a Γ\Gamma-invariant interval.

Suppose now that XX is of finite dimension DD and that Γ\Gamma is not necessarily amenable but preserves an interval X¯\mathcal{I}\subset\overline{X}. By Corollary 0.4 (see also [Fer18, Corollary 2.9]), the number of end points on which \mathcal{I} is an interval is 2D2^{D^{\prime}} for some 0DD0\leqslant{D^{\prime}}\leqslant D and we identify these with (/2)D{0,1}D\left({\mathbb{Z}/2\mathbb{Z}}\right)^{D^{\prime}}\cong\{0,1\}^{D^{\prime}}. By [CS11, Proposition 2.6] we have that Aut({0,1}D){0,1}DSym(D)\text{Aut}\,(\{0,1\}^{D^{\prime}})\cong\{0,1\}^{D^{\prime}}\rtimes\mathrm{Sym}({D^{\prime}}). We may therefore project ΓAut({0,1}D)\Gamma\to\text{Aut}\,(\{0,1\}^{D^{\prime}}), and without loss of generality, assume ΓAut({0,1}D)\Gamma\leqslant\text{Aut}\,(\{0,1\}^{D^{\prime}}).

Let Γ0=Γ{0,1}DΓ\Gamma_{0}=\Gamma\cap\{0,1\}^{D^{\prime}}\lhd\Gamma and note that |Γ0|=2N|\Gamma_{0}|=2^{N} for some 0ND0\leqslant N\leqslant{D^{\prime}}. Fix a choice of right Γ0\Gamma_{0}-coset representatives SΓS\subset\Gamma, with trivial {0,1}D\{0,1\}^{D^{\prime}}-coordinate. Let 𝒪{0,1}D\mathcal{O}\in\{0,1\}^{D^{\prime}} be defined component-wise by 𝒪i0\mathcal{O}_{i}\equiv 0, for i{1,,D}i\in\{1,\dots,D^{\prime}\}. Note that 𝒪\mathcal{O} is fixed by Sym(D)\mathrm{Sym}({D^{\prime}}) and has trivial stabilizer in Γ0\Gamma_{0}. Let (𝒪,α)S(\mathcal{O},\alpha)\in S. Then Γ0(𝒪,α).𝒪=Γ0.𝒪\Gamma_{0}(\mathcal{O},\alpha).\mathcal{O}=\Gamma_{0}.\mathcal{O}. We have shown that

Γ.𝒪=(𝒪,α)SΓ0(𝒪,α).𝒪=Γ0.𝒪\Gamma.\mathcal{O}=\underset{(\mathcal{O},\alpha)\in S}{\sqcup}\Gamma_{0}(\mathcal{O},\alpha).\mathcal{O}=\Gamma_{0}.\mathcal{O}

Therefore, by the orbit stabilizer theorem, we have

|Γ.𝒪|=|Γ0.𝒪|=|Γ0|/|stabΓ0(𝒪)|=2N.|\Gamma.\mathcal{O}|=|\Gamma_{0}.\mathcal{O}|=|\Gamma_{0}|/|\mathrm{stab}_{\Gamma_{0}}(\mathcal{O})|=2^{N}.
[Uncaptioned image]

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