On the stability of hyperbolicity under quantitative measure equivalence
Thiebout Delabie, Juhani Koivisto, François Le Maître, Romain Tessera
TL;DR
The paper investigates the stability of hyperbolicity under quantitative measure equivalence between finitely generated groups. It proves that a cobounded $(\mathrm{L}^p,\mathrm{L}^{\infty})$ measure equivalence coupling from a hyperbolic group $\Gamma$ to a group $\Lambda$ enforces hyperbolicity of $\Lambda$ for a threshold $p>108\delta\mathrm{Ent}(S_\Gamma)+2$, with the bound depending on the hyperbolicity constant $\delta$ and the volume entropy $\mathrm{Ent}(S_\Gamma)$. It extends to more general $(\varphi,\psi)$-integrable couplings, showing rigidity under exponential-polynomial trade-offs and highlighting a sharp contrast with higher-rank lattices where exponentials dominate. The argument combines a geometric obstruction based on embedded cycles in non-hyperbolic spaces with cocycle estimates arising from the ME coupling, and leverages coboundedness to relate fundamental domains. Overall, the work demonstrates a strong form of hyperbolicity rigidity under quantitative orbit/measure equivalence and yields concrete corollaries for rank-one lattices and OE settings.
Abstract
A well-known result of Shalom says that lattices in SO$(n,1)$ are $\mathrm{L}^p$ measure equivalent for all $p<n-1$. His proof actually yields the following stronger statement: the natural coupling resulting from a suitable choice of fundamental domains from a uniform lattice to a non-uniform one is $(\mathrm{L}^p,\mathrm{L}^{\infty})$. Moreover, it is easy to see that the coupling is cobounded: the fundamental domain of the uniform lattice is contained in a union of finitely many translates of the fundamental domain of the non-uniform one. The purpose of this note is to prove that this statement is sharp in the following sense: if a ME-coupling from a hyperbolic group to a non-hyperbolic group is cobounded and $(\mathrm{L}^p,\mathrm{L}^{\infty})$, then $p$ must be less than some $p_0$ only depending on the hyperbolic group.
