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Thin right-angled Coxeter groups in some uniform arithmetic lattices

Sami Douba McGill University, Department of Mathematics and Statistics sami.douba@mail.mcgill.ca
Abstract.

Using a variant of an unpublished argument due to Agol, we show that an irreducible right-angled Coxeter group on n3{n\geq 3} vertices embeds as a thin subgroup of a uniform arithmetic lattice in an indefinite orthogonal group O(p,q)\mathrm{O}(p,q) for some p,q1p,q\geq 1 satisfying p+q=np+q=n.

The author was supported by a public grant as part of the Investissement d’avenir project, FMJH, and by the National Science Centre, Poland UMO-2018/30/M/ST1/00668.

Let 𝐆{\bf G} be a semisimple algebraic \mathbb{R}-group and Γ\Gamma a lattice in G:=𝐆()G:={\bf G}(\mathbb{R}). A subgroup ΔΓ\Delta\subset\Gamma is said to be thin if Δ\Delta is Zariski-dense in GG but of infinite index in Γ\Gamma. It follows from the Borel density theorem [Bor60, Corollary 4.3] and a classical result of Tits [Tit72, Theorem 3] that if 𝐆{\bf G} as above is nontrivial, connected, and without compact factors, then any lattice in GG contains a thin nonabelian free subgroup. A famous construction of Kahn–Markovic [KM12] produces thin surface subgroups of all uniform lattices in SO(3,1)\mathrm{SO}(3,1) (see [Ham15], [LR16], [CF19], [KLM18] for some other manifestations of surface groups as thin groups). In [BL20], Ballas–Long show that many arithmetic lattices in SO(n,1)\mathrm{SO}(n,1) virtually embed as thin subgroups of lattices in SLn+1()\mathrm{SL}_{n+1}(\mathbb{R}), and raise the question as to which groups arise as thin groups. In this note, we observe the following.

Theorem 1.

An irreducible right-angled Coxeter group on n3n\geq 3 vertices embeds as a thin subgroup of a uniform arithmetic lattice in O(p,q)\mathrm{O}(p,q) for some p,q1p,q\geq 1 satisfying p+q=np+q=n.

To that end, let Σ1\Sigma_{1} be a connected simplicial graph on n3n\geq 3 vertices; we think of Σ1\Sigma_{1} as a Coxeter diagram in the sense of [FT14, Section 2.1] all of whose edges are bold. Fix an order v1,,vnv_{1},\ldots,v_{n} on the vertices of Σ1\Sigma_{1}, and let WW be the group given by the presentation with generators γ1,,γn\gamma_{1},\ldots,\gamma_{n} subject to the relations γi2=1\gamma_{i}^{2}=1 for i=1,,ni=1,\ldots,n, and [γi,γj]=1[\gamma_{i},\gamma_{j}]=1 for each distinct i,j{1,n}i,j\in\{1,\ldots n\} such that viv_{i} and vjv_{j} are not adjacent in Σ1\Sigma_{1}. The group WW is the (right-angled) Coxeter group associated to the diagram Σ1\Sigma_{1}. Let W+W^{+} be the index-22 subgroup of WW consisting of all elements that can be expressed as a product of an even number of the γi\gamma_{i}; that W+W^{+} indeed constitutes an index-22 subgroup of WW follows, for instance, from faithfulness of the representation σ1\sigma_{1} of WW to be defined in the sequel.

For dd\in\mathbb{R}, let Md=(mij)Mn([d])M_{d}=(m_{ij})\in\mathrm{M}_{n}(\mathbb{Z}[d]) be the symmetric matrix given by

mij={1if i=jdif ij and vi,vj are joined by an edge in Σ10otherwise.m_{ij}=\begin{cases}1&\text{if }i=j\\ -d&\text{if }i\neq j\text{ and }v_{i},v_{j}\text{ are joined by an edge in }\Sigma_{1}\\ 0&\text{otherwise.}\end{cases}

Let ϵ>0\epsilon>0 be such that MdM_{d} is positive-definite for d[ϵ,ϵ]d\in[-\epsilon,\epsilon], and let D1D\geq 1 be such that MdM_{d} is nondegenerate and its signature constant as dd varies within [D,)[D,\infty). Note that M1M_{1} is the Gram matrix of the diagram Σ1\Sigma_{1} (and the given order on the vertices of Σ1\Sigma_{1}). In particular, we have that ϵ<1\epsilon<1. For d>1d>1, the matrix MdM_{d} is the Gram matrix of the diagram Σd\Sigma_{d} obtained from Σ1\Sigma_{1} by replacing each edge with a dotted edge labeled by dd. (Here, we are again using the conventions employed by [FT14, Section 2.1].)

For d1d\geq 1, let σd:WGLn()\sigma_{d}:W\rightarrow\mathrm{GL}_{n}(\mathbb{R}) be the Tits–Vinberg representation associated to the Coxeter diagram Σd\Sigma_{d} and the given order on its vertices; this is the representation given by

σd(γi)(v)=v2(vTMdei)ei\sigma_{d}(\gamma_{i})(v)=v-2(v^{T}M_{d}e_{i})e_{i}

for i=1,,ni=1,\ldots,n and vnv\in\mathbb{R}^{n}, where (e1,,en)(e_{1},\ldots,e_{n}) is the standard basis for n\mathbb{R}^{n}. It follows from Vinberg’s theory of reflection groups that the representations σd\sigma_{d}, d1d\geq 1, are faithful [Vin71, Theorem 5] (see Lecture 1 in [Ben04] for an exposition). This family of representations was studied in [DGK20].

If MMn()M\in\mathrm{M}_{n}(\mathbb{R}) is a symmetric matrix and AA is a subdomain of \mathbb{C}, we write

O(M;A)\displaystyle\mathrm{O}(M;A) ={gGLn(A):gTMg=M},\displaystyle=\{g\in\mathrm{GL}_{n}(A)\>:\>g^{T}Mg=M\},
SO(M;A)\displaystyle\mathrm{SO}(M;A) ={gSLn(A):gTMg=M}.\displaystyle=\{g\in\mathrm{SL}_{n}(A)\>:\>g^{T}Mg=M\}.

Note that we have Wd:=σd(W)O(Md;)W_{d}:=\sigma_{d}(W)\subset\mathrm{O}(M_{d};\mathbb{R}) by design.

Lemma 2.

The group WdW_{d} is Zariski-dense in O(Md;)\mathrm{O}(M_{d};\mathbb{R}) for dDd\geq D.

Proof.

The proof of the main theorem in [BdlH04] applies here, so we only sketch the argument provided there. Let dDd\geq D and let GdG_{d} be the Zariski-closure of WdW_{d} in O(Md;)\mathrm{O}(M_{d};\mathbb{R}). Denote by 𝔤\mathfrak{g} and 𝔥\mathfrak{h} the Lie algebras of O(Md;)\mathrm{O}(M_{d};\mathbb{R}) and GdG_{d}, respectively. It is enough to show that 𝔤=𝔥\mathfrak{g}=\mathfrak{h}, since the Zariski-closure of SO(Md;)\mathrm{SO}(M_{d};\mathbb{R})^{\circ} is SO(Md;)\mathrm{SO}(M_{d};\mathbb{R}) and since WdSO(Md;)W_{d}\not\subset\mathrm{SO}(M_{d};\mathbb{R}).

For each distinct pair i,j{1,,n}i,j\in\{1,\ldots,n\}, let Ei,jE_{i,j} be the orthogonal complement of ei,ej\langle e_{i},e_{j}\rangle in n\mathbb{R}^{n} with respect to MdM_{d}. The subgroup of O(Md;)\mathrm{O}(M_{d};\mathbb{R}) consisting of all elements that fix each vector in Ei,jE_{i,j} is a 11-dimensional closed subgroup of O(Md;)\mathrm{O}(M_{d};\mathbb{R}) whose identity component Ti,jT_{i,j} corresponds to a subspace Xi,j\langle X_{i,j}\rangle of 𝔤\mathfrak{g} for some Xi,j𝔤{X_{i,j}\in\mathfrak{g}}. Since MdM_{d} is nondegenerate, the elements Xi,jX_{i,j} form a basis for 𝔤\mathfrak{g} as a vector space [BdlH04, Lemme 7]. Thus, to show 𝔤=𝔥\mathfrak{g}=\mathfrak{h}, it suffices to show that Xi,j𝔥X_{i,j}\in\mathfrak{h} for each distinct pair i,j{1,,n}i,j\in\{1,\ldots,n\}.

To that end, let i,j{1,,n}i,j\in\{1,\ldots,n\}, iji\neq j, and suppose first that viv_{i} and vjv_{j} are adjacent in Σ1\Sigma_{1}. Then σd(γiγj)\sigma_{d}(\gamma_{i}\gamma_{j}) generates an infinite cyclic subgroup of Ti,jT_{i,j}, so that Ti,jGdT_{i,j}\subset G_{d}. It follows that Xi,j𝔥X_{i,j}\in\mathfrak{h} in this case. One now verifies that, since Σ1\Sigma_{1} is connected, any Lie subalgebra of 𝔤\mathfrak{g} that contains Xi,jX_{i,j} for all i,ji,j such that vi,vjv_{i},v_{j} are adjacent in fact contains Xi,jX_{i,j} for each distinct pair i,j{1,,n}i,j\in\{1,\ldots,n\} [BdlH04, Preuve du Théorème, second cas]. ∎

Now let KK\subset\mathbb{R} be a real quadratic extension of \mathbb{Q}, let τ:KK\tau:K\rightarrow K be the nontrivial element of Gal(K/)\mathrm{Gal}(K/\mathbb{Q}), and let 𝒪K\mathcal{O}_{K} be the ring of integers of KK. Then by Dirichlet’s unit theorem, there is a unit α𝒪K\alpha\in\mathcal{O}_{K}^{*} such that αmax{1ϵ,D}\alpha\geq\max\{\frac{1}{\epsilon},D\}. Thus, we have

|τ(α)|ϵα|τ(α)|=|ατ(α)|=1,\frac{|\tau(\alpha)|}{\epsilon}\leq\alpha|\tau(\alpha)|=|\alpha\cdot\tau(\alpha)|=1,

where the final equality holds because α𝒪K\alpha\in\mathcal{O}_{K}^{*}. We conclude that |τ(α)|ϵ|\tau(\alpha)|\leq\epsilon, and so Mτ(α)M_{\tau(\alpha)} is positive-definite. It follows that Γ:=O(Mα;𝒪K)\Gamma:=\mathrm{O}(M_{\alpha};\mathcal{O}_{K}) is a uniform arithmetic lattice in O(Mα;)\mathrm{O}(M_{\alpha};\mathbb{R}) (for an efficient survey of the relevant facts, see, for instance, Section 2 of [GPS87]). Moreover, we have WαO(Mα;[α])ΓW_{\alpha}\subset\mathrm{O}(M_{\alpha};\mathbb{Z}[\alpha])\subset\Gamma.

Remark 3.

Note that Galois conjugation by τ\tau transports Γ\Gamma and hence WαW_{\alpha} into the compact group O(Mτ(α);)\mathrm{O}(M_{\tau(\alpha)};\mathbb{R}). That right-angled Coxeter groups on finitely many vertices embed in compact Lie groups had already been observed by Agol [Ago18] using a similar trick to the one above. Indeed, Agol’s argument was the inspiration for this note.

Proof of Theorem 1.

We show that WαW_{\alpha} is a thin subgroup of ΓO(Mα;)\Gamma\subset\mathrm{O}(M_{\alpha};\mathbb{R}). By Lemma 2, it suffices to show that WαW_{\alpha} is of infinite index in Γ\Gamma. Indeed, suppose otherwise. Then WαW_{\alpha} is a uniform lattice in O(Mα;)\mathrm{O}(M_{\alpha};\mathbb{R}). If n=3n=3, then immediately we obtain a contradiction, since in this case WαW_{\alpha} is virtually a closed hyperbolic surface group, whereas WW is virtually free. Now suppose n>3n>3. There is some β>α\beta>\alpha and a path [α,β]GLn(),dhd[\alpha,\beta]\rightarrow\mathrm{GL}_{n}(\mathbb{R}),d\mapsto h_{d} such that hdTMdhd=Mαh_{d}^{T}M_{d}h_{d}=M_{\alpha} for all d[α,β]d\in[\alpha,\beta] (this follows, for example, from the fact that GLn()\mathrm{GL}_{n}(\mathbb{R}) acts continuously and transitively on the set ΩMn()\Omega\subset M_{n}(\mathbb{R}) of symmetric matrices with the same signature as MαM_{\alpha}, and so the orbit map GLn()Ω,ggTMαg\mathrm{GL}_{n}(\mathbb{R})\rightarrow\Omega,g\mapsto g^{T}M_{\alpha}g is a fiber bundle). Setting gd=hdhα1g_{d}=h_{d}h_{\alpha}^{-1} for d[α,β]d\in[\alpha,\beta], we have that gα=Ing_{\alpha}=I_{n} and gdTMdgd=Mαg_{d}^{T}M_{d}g_{d}=M_{\alpha} for d[α,β]d\in[\alpha,\beta]. For d[α,β]d\in[\alpha,\beta], let ρd=gd1σdgd\rho_{d}=g_{d}^{-1}\sigma_{d}g_{d}, and note ρd(W)gd1O(Md;)gd=O(gdTMdgd;)=O(Mα;)\rho_{d}(W)\subset g_{d}^{-1}\mathrm{O}(M_{d};\mathbb{R})g_{d}=\mathrm{O}(g_{d}^{T}M_{d}g_{d};\mathbb{R})=\mathrm{O}(M_{\alpha};\mathbb{R}).

Let ρd+=ρd|W+\rho_{d}^{+}=\rho_{d}\bigr{|}_{W^{+}} and σd+=σd|W+\sigma_{d}^{+}=\sigma_{d}\bigr{|}_{W^{+}} for d[α,β]d\in[\alpha,\beta]. Then ρα+(W+)\rho_{\alpha}^{+}(W^{+}) is a uniform lattice in the connected non-compact simple Lie group SO(Mα;)\mathrm{SO}(M_{\alpha};\mathbb{R})^{\circ}, and the latter is not locally isomorphic to SO(2,1)\mathrm{SO}(2,1)^{\circ} by our assumption that n>3n>3. Thus, by Weil local rigidity [Wei60, Wei62], up to choosing β\beta closer to α\alpha, we may assume that for each d[α,β]d\in[\alpha,\beta] there is some adSO(Mα;)a_{d}\in\mathrm{SO}(M_{\alpha};\mathbb{R})^{\circ} such that

(1) ρd+=adρα+ad1=adσα+ad1.\rho_{d}^{+}=a_{d}\rho_{\alpha}^{+}a_{d}^{-1}=a_{d}\sigma_{\alpha}^{+}a_{d}^{-1}.

But ρd+=gd1σd+gd\rho_{d}^{+}=g_{d}^{-1}\sigma_{d}^{+}g_{d}, so we obtain from (1) that the trace tr(σd(γiγj))\mathrm{tr}(\sigma_{d}(\gamma_{i}\gamma_{j})) remains constant as dd varies within [α,β][\alpha,\beta], where i,j{1,,n}i,j\in\{1,\ldots,n\} are chosen so that the vertices vi,vjv_{i},v_{j} are adjacent in Σ1\Sigma_{1}.

We claim, however, that tr(σd(γiγj))=4d24+n\mathrm{tr}(\sigma_{d}(\gamma_{i}\gamma_{j}))=4d^{2}-4+n for dDd\geq D. Indeed, let dDd\geq D. Then MdM_{d} is nondegenerate, so that d\mathbb{R}^{d} splits as a direct sum of the 22-dimensional subspace ei,ejn\langle e_{i},e_{j}\rangle\subset\mathbb{R}^{n} and its orthogonal complement Ei,jE_{i,j} with respect to MdM_{d}. Each of γi\gamma_{i} and γj\gamma_{j} acts as the identity on Ei,jE_{i,j}, so our claim is equivalent to the assertion that tr(σd(γiγj)|ei,ej)=4d22\mathrm{tr}\left(\sigma_{d}(\gamma_{i}\gamma_{j})\bigr{|}_{\langle e_{i},e_{j}\rangle}\right)=4d^{2}-2, and the latter follows from the fact that, with respect to the basis (ei,ej)(e_{i},e_{j}) of ei,ej{\langle e_{i},e_{j}\rangle}, the matrices representing σd(γi),σd(γj)\sigma_{d}(\gamma_{i}),\sigma_{d}(\gamma_{j}) are (12d01),(102d1),\begin{pmatrix}-1&2d\\ 0&1\end{pmatrix},\begin{pmatrix}1&0\\ 2d&-1\end{pmatrix}, respectively. ∎

Example 4.

We consider the case that n5n\geq 5 and the complement graph of Σ1\Sigma_{1} is the cycle v1v2vnv_{1}v_{2}\ldots v_{n}. In this case, the group WW may be realized as the subgroup of Isom(2)\mathrm{Isom}(\mathbb{H}^{2}) generated by the reflections in the sides of a regular right-angled hyperbolic nn-gon, so that WW is virtually the fundamental group of a closed hyperbolic surface. We have

(2) Md=(1+d)In+d(Jn+Jnn1)d(In+Jn++Jnn1)M_{d}=(1+d)I_{n}+d(J_{n}+J_{n}^{n-1})-d(I_{n}+J_{n}+\ldots+J_{n}^{n-1})

where JnMn()J_{n}\in\mathrm{M}_{n}(\mathbb{C}) is the matrix

Jn=(e2e3ene1).J_{n}=\begin{pmatrix}e_{2}&e_{3}&\ldots&e_{n}&e_{1}\end{pmatrix}.

There is some CGLn()C\in\mathrm{GL}_{n}(\mathbb{C}) such that

CJnC1=diag(1,ζn,ζn2,,ζnn1)CJ_{n}C^{-1}=\mathrm{diag}(1,\zeta_{n},\zeta_{n}^{2},\ldots,\zeta_{n}^{n-1})

where ζn=e2πi/n\zeta_{n}=e^{2\pi i/n}. Observe that

C(In+Jn++Jnn1)C1\displaystyle C(I_{n}+J_{n}+\ldots+J_{n}^{n-1})C^{-1} =diag(n,0,,0)\displaystyle=\mathrm{diag}(n,0,\ldots,0)
C(Jn+Jnn1)C1\displaystyle C(J_{n}+J_{n}^{n-1})C^{-1} =diag(2,2cos2πn,2cos2π2n,,2cos2π(n1)n).\displaystyle=\mathrm{diag}\left(2,2\cos\frac{2\pi}{n},2\cos\frac{2\pi\cdot 2}{n},\ldots,2\cos\frac{2\pi(n-1)}{n}\right).

It follows from (2) that, counted with multiplicity, the eigenvalues of MdM_{d} are 1d(n3){1-d(n-3)} and 1+d(1+2cos2πkn)1+d\left(1+2\cos\frac{2\pi k}{n}\right), where k=1,,n1k=1,\ldots,n-1. Note that for dd sufficiently large, we have that 1d(n3)<01-d(n-3)<0, and that 1+d(1+2cos2πkn)01+d\left(1+2\cos\frac{2\pi k}{n}\right)\geq 0 if and only if cos2πkn12\cos\frac{2\pi k}{n}\geq-\frac{1}{2}. We conclude that the signature of MdM_{d} is (2n3,n2n3)(2\lfloor\frac{n}{3}\rfloor,n-2\lfloor\frac{n}{3}\rfloor) for all dd sufficiently large. In particular, if n=3mn=3m, m2m\geq 2, then the signature of MdM_{d} is (2m,m)(2m,m) for all dd sufficiently large. The above discussion yields thin surface subgroups of uniform arithmetic lattices in SO(2n3,n2n3)\mathrm{SO}(2\lfloor\frac{n}{3}\rfloor,n-2\lfloor\frac{n}{3}\rfloor) for each n5n\geq 5.

Acknowledgements

I thank Yves Benoist and Pierre Pansu for helpful discussions. I am also deeply grateful to the latter for inviting me to spend the fall of 2021 at Université Paris-Saclay, where this note was written, and to my supervisor Piotr Przytycki for his support during my stay.

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