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Furstenberg entropy of intersectional invariant random subgroups

Published online by Cambridge University Press:  17 September 2018

Yair Hartman
Affiliation:
Department of Mathematics, Northwestern University, 2033 Sheridan Road, Evanston, IL 60208-2730, USA email hartman@math.northwestern.edu
Ariel Yadin
Affiliation:
Department of Mathematics, Ben Gurion University of the Negev, P.O.B. 653, 8410501 Be’er Sheva, Israel email yadina@bgu.ac.il
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Abstract

We study the Furstenberg-entropy realization problem for stationary actions. It is shown that for finitely supported probability measures on free groups, any a priori possible entropy value can be realized as the entropy of an ergodic stationary action. This generalizes results of Bowen. The stationary actions we construct arise via invariant random subgroups (IRSs), based on ideas of Bowen and Kaimanovich. We provide a general framework for constructing a continuum of ergodic IRSs for a discrete group under some algebraic conditions, which gives a continuum of entropy values. Our tools apply, for example, for certain extensions of the group of finitely supported permutations and lamplighter groups, hence establishing full realization results for these groups. For the free group, we construct the IRSs via a geometric construction of subgroups, by describing their Schreier graphs. The analysis of the entropy of these spaces is obtained by studying the random walk on the appropriate Schreier graphs.

Information

Type
Research Article
Copyright
© The Authors 2018 
Figure 0

Figure 1. Part of the labeled graph ${\mathcal{N}}_{a}$.

Figure 1

Figure 2. The subgraph $(\mathbb{F}_{2})_{{\leqslant}3}$. Edges labeled $a$ are dotted and labeled $b$ are solid. The vertices $x,y,z,w$ are $a,a^{-1},b,b^{-1}$-leaves respectively.

Figure 2

Figure 3. A visualization of gluing $(\unicode[STIX]{x1D6EC},\unicode[STIX]{x1D716})$ to $(\mathbb{F}_{2})_{{\leqslant}3}$. The dotted edges correspond to the label $a$, and the full edges to $b$. The vertex $g$ is an $a$-leaf. Thus, a copy of $\unicode[STIX]{x1D6EC}$, denoted $\unicode[STIX]{x1D6EC}_{g}$ is connected by removing the edge $\unicode[STIX]{x1D716}$ (dashed) and adding to edges $(x_{g},g),(g,y_{g})$ labeled $b$ (solid). A copy of ${\mathcal{N}}_{a}$, denoted ${\mathcal{N}}_{g}$, is connected via an edge $(0_{g},g)$ labeled $a$ (dotted). Also, to the $b$-leaf $\unicode[STIX]{x1D6FE}$, a copy of ${\mathcal{N}}_{b}$, denoted ${\mathcal{N}}_{\unicode[STIX]{x1D6FE}}$ is added via an edge $(0_{\unicode[STIX]{x1D6FE}},\unicode[STIX]{x1D6FE})$ labeled $b$ (full), and an additional self-loop labeled $a$ (dotted) is added at $\unicode[STIX]{x1D6FE}$.