As hyperbolic as they Comm

Nir Lazarovich is the speaker. He works at Technion in Israel. I am attending this seminar at the mathematics department at TIFR.

Introduction

\(\Gamma\) a f.g. group is hyperbolic if it is \(X = \mathrm{Cay}(\Gamma,S)\) is hyperbolic, where \(\langle S\rangle = \Gamma\) is a finite generating set. The Cayley tree being hyperbolic is equivalent to \[\begin{equation} \exists \delta > 0, \ \forall x,y,z \in X, [x,z] \subseteq N_{\delta} ( [x,y] \cup [y,z]). \end{equation}\] Here \([x,y]\) is the shortest path between \(x,y\) and \(N_{\delta}(A)\) is the \(\delta\)-neighbourhood of a set \(A\).

Motivation

Examples

Just to get out of the way, \(\Gamma\) is always torsion free for the rest of this talk.

Here are some examples.

Some results

(Sela)

  1. If \(\Gamma\) is 1-ended hyperbolic, then \(\Gamma\) is co-Hopfian: i.e. \(\Gamma\) is not isomorphic to a proper subgroup of itself. 1

(Sela)

  1. If \(\Gamma\) is normal in \(G\), and both \(\Gamma\) and \(G\) are torsion-free hyperbolic, then \(\Gamma\) is a free product of surface and free groups.

(Paulin)

  1. If \(\Gamma\) is hyperbolic and does not split over \(\mathbb{Z}\) then \(|\mathrm{Out}(\Gamma)|< \infty\).

A (abstract) commensurator of \(\Gamma\) is an isomorphism \(\varphi: H_{1} \xrightarrow[\simeq]{} H_{2}\) such that \(H_{1} \subseteq \Gamma\), \(| \Gamma : H_{i}| < \infty\). Here both \(H_{1}, H_{2}\) are some subgroups of \(\Gamma\).

(Whyte)

Can \(1\)-ended hyperbolic group \(\Gamma\) have \(H_{1} \simeq H_{2} < \Gamma\) of different indices?

(Stark-Woodhouse)

Yes, \(\exists \Gamma\) 1-end hyperbolic such that \[\begin{equation} H_{1} \simeq H_{2} \leq \Gamma \text{ such that } [\Gamma: H_{1} ] < \infty \text{ and }[\Gamma : H_{2}] = \infty \end{equation}\]

\(\Gamma\) is a finite index rigid if \(\forall H_{1} , H_{2} \subseteq \Gamma\) of finite index if \(H_{1} \simeq H_{2} \implies [\Gamma: H_{1}] = [\Gamma : H_{2}]\).

\(\mathbb{Z}\) is not f.i.r because \(\mathbb{Z} \simeq 2 \mathbb{Z}\).

(L., 2023)

If \(\Gamma\) is hyperbolic non-elementary then \(\Gamma\) is f.i.r.

(L.-Rahamain-Sisto, 25)

\(\mathbb{Z} \simeq \Gamma\) is t.f. hyperbolic relative to type \(F\) NRH proper subgroups, then \(\Gamma\) is f.i.r.

\(\Gamma \leq G\) then \(\mathrm{Comm}_{G}(\Gamma)\) is defined as \[\begin{equation} \mathrm{Comm}_{G}(\Gamma) = \{ g\in G \mid [\Gamma : \Gamma \cap g \Gamma g^{-1}] < \infty, [g \Gamma g^{-1}, \Gamma \cap g \Gamma g^{-1} ] < \infty\}. \end{equation}\] We also define \[\begin{equation} \mathrm{N}_{G}(\Gamma) = \{ g\in G \mid g \Gamma g^{-1} = \Gamma \} \end{equation}\]

\[\begin{equation} \Gamma \text{ is normal in } G \Leftrightarrow N_{G}(\Gamma) = G \end{equation}\]

\(\Gamma\) be almost normal subgroup in \(G\) if \(\mathrm{Comm}_{G}(\Gamma) = G\): aka commensurated subgroups.

There is an example of this given by \[\begin{equation} G = \langle a, t \mid t a^{p} t^{-1} = a^{q}\rangle. \end{equation}\] Here the subgroup \(\Gamma = \langle a\rangle\) is almost normal.

If \(G\) is finitely generated, one has \[\begin{equation} \Gamma \text{ almost normal in } G \Leftrightarrow \Gamma - \mathrm{Stab}_{G}(v) \text{ for an action } G \curvearrowright\underbrace{Y}_{\text{ hc. finite graph}.} \end{equation}\]

(L-Margolis-Mj)

If \(\Gamma\) is almost normal in \(G\) and both \(\Gamma\) and \(G\) are torsion-free hyperbolic, then \(\Gamma\) is a free product of surface and free groups.

(Then there was a sketch of the proof which was a bit too technical for me)

Commutator of a group

\[\begin{equation} \mathrm{Comm}(\Gamma) = \{ \phi : H_{1} \xrightarrow[\simeq]{} H_{2} \mid H_{i} \leq_{ \text{ f.i. }} \Gamma \} / \sim \end{equation}\] A priori \(\mathrm{Comm}(\Gamma)\) is a groupoid but by passing to subgroup \(H_{1} \cap H_{2}\) which are finite index in both \(H_{1},H_{2}\) one can compose maps. Therefore this becomes a group.

For example, \[\begin{equation} \mathrm{Comm}(\mathbb{Z}) \simeq \mathbb{Q}^{\times}. \end{equation}\] To see this, observe that \(q \mathbb{Z} \rightarrow p \mathbb{Z}\) is the map \(x \mapsto \pm \tfrac{p}{q} x\).
\[\begin{equation} \underbrace{\pi_{1} ( \text{ closed hyperbolic $3$-manifolds })}_{\Gamma} \leq \mathrm{PSL}_{2}(\mathbb{C}) \end{equation}\]
\[\begin{equation} \mathrm{Comm}_{\mathrm{PSL}_{2}(\mathbb{C})}( \mathrm{PSL}_{2}(\mathbb{Z})) \geq \mathrm{PSL}_{2}(\mathbb{Q}) \end{equation}\]
\(\Gamma\) is rigid \(\implies\) \((\mathrm{Comm}(\Gamma) : \mathrm{Inn}(\Gamma)) < \infty\)

The answer is negative. The example of \(\mathrm{PSL}_{2}(\mathbb{Z})\) is supposed to illustrate this.

(Mostow rigidity):

For \[\begin{equation} \Gamma = \pi_{1}( \text{ closed hyperbolic 3-manifold}), \end{equation}\] one has \[\begin{equation} \mathrm{Comm}(\Gamma) = \mathrm{Comm}_{\mathrm{PSL}_{2}(\mathbb{C})} (\Gamma) \end{equation}\]

(Gromov)

\(\Gamma\) rigid hyperbolic then \(\exists\) locally compact topological \(G\) s.t. \(\Gamma \leq G\) is a discrete cocompact and \(\mathrm{Comm}_{G}(\Gamma) = \mathrm{Comm}(\Gamma)\).


  1. Nir adds: the condition of being 1-ended, under the assumption of torsion-free, is the same as freely-indecomposable.↩︎


This page was updated on February 6, 2026.
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