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Entropy, products, and bounded orbit equivalence

Published online by Cambridge University Press:  06 December 2021

DAVID KERR*
Affiliation:
Mathematisches Institut, WWU Münster, Einsteinstr. 62, Münster 48149, Germany
HANFENG LI
Affiliation:
Center of Mathematics, Chongqing University, Chongqing 401331, China Department of Mathematics, SUNY at Buffalo, Buffalo, NY 14260-2900, USA (e-mail: [email protected])
*
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Abstract

We prove that if two topologically free and entropy regular actions of countable sofic groups on compact metrizable spaces are continuously orbit equivalent, and each group either (i) contains a w-normal amenable subgroup which is neither locally finite nor virtually cyclic, or (ii) is a non-locally-finite product of two infinite groups, then the actions have the same sofic topological entropy. This fact is then used to show that if two free uniquely ergodic and entropy regular probability-measure-preserving actions of such groups are boundedly orbit equivalent then the actions have the same sofic measure entropy. Our arguments are based on a relativization of property SC to sofic approximations and yield more general entropy inequalities.

Type
Original Article
Creative Commons
Creative Common License - CCCreative Common License - BY
This is an Open Access article, distributed under the terms of the Creative Commons Attribution licence (http://creativecommons.org/licenses/by/4.0), which permits unrestricted re-use, distribution and reproduction, provided the original article is properly cited.
Copyright
© The Author(s), 2021. Published by Cambridge University Press

1 Introduction

At first glance it may seem that dynamical entropy and orbit equivalence should have little to do with one another. One is a conjugacy invariant that is tailor-made for the hairsplitting job of distinguishing Bernoulli shifts, all of which have the same spectral theory, while the other is a coarse relation between group actions whose tendency to nullify asymptotic behaviour is most devastating in the setting of amenable groups, where entropy finds its classical home [Reference Dye10, Reference Kolmogorov26, Reference Kolmogorov27, Reference Ornstein and Weiss34, Reference Sinai41]. One registers information, while the other threatens to destroy it.

This brutal disparity can, however, be honed so as to bring the two concepts into frequent and sometimes surprising alignment. Indeed, entropy turns out to be sensitive in meaningful ways to the various kinds of restrictions that one may naturally impose on an orbit equivalence, its role as an invariant remaining intact in some cases but completely neutralized in others. The history of this relationship traces back several decades and in its original thrust encompasses the work of Vershik on actions of locally finite groups [Reference Vershik42, Reference Vershik43], the Ornstein isomorphism machinery for Bernoulli shifts [Reference Ornstein32], the theory of Kakutani equivalence [Reference del Junco and Rudolph9, Reference Feldman11, Reference Katok19, Reference Ornstein, Rudolph and Weiss33], and Kammeyer and Rudolph’s general theory of restricted orbit equivalence for probability-measure-preserving (p.m.p.) actions of countable amenable groups that all of this inspired [Reference Kammeyer and Rudolph17, Reference Kammeyer and Rudolph18, Reference Rudolph37] (see [Reference Kammeyer and Rudolph18, Ch. 1] for a genealogy). In a somewhat different vein from these lines of investigation, Rudolph and Weiss later proved in [Reference Rudolph and Weiss38] that, for a free p.m.p. action of a countable amenable group, the conditional entropy with respect to a prescribed invariant sub- $\sigma $ -algebra ${\mathscr S}$ is preserved under every ${\mathscr S}$ -measurable orbit equivalence. As Rudolph and Weiss demonstrated in the application to completely positive entropy that motivated their paper, this crisp expression of complementarity between entropy and orbit equivalence, when combined with the Ornstein–Weiss theorem [Reference Ornstein and Weiss34], turns out to be very useful as a tool for lifting results from ${\mathbb Z}$ -actions to actions of general countable amenable groups. More recently Austin has shown, for free p.m.p. actions of finitely generated amenable groups, that entropy is an invariant of bounded and integrable orbit equivalence, and that there is an entropy scaling formula for stable versions of these equivalences [Reference Austin3]. It is interesting to note that Austin makes use of both the theory of Kakutani equivalence (to handle the virtually cyclic case, which his approach requires him to treat separately) and the Rudolph–Weiss theorem (in a reduction-to- ${\mathbb Z}$ argument which, ironically, forms part of the verification of the non-virtually-cyclic case).

The basic geometric idea at play in Austin’s work when the group is not virtually cyclic is the possibility of finding, within suitable connected Følner subsets of the group, a connected subgraph which is sparse but at the same time dense at a specified coarse scale. By recasting this sparse connectivity as a condition on the action that we called property SC and circumventing the ‘derandomization’ of [Reference Austin3] with its reliance on the Rudolph–Weiss technique, we established in [Reference Kerr and Li25] the following extension beyond the amenable setting: if G is a countable group containing a w-normal amenable subgroup which is neither locally finite nor virtually cyclic, H is a countable group, and $G\curvearrowright (X,\mu )$ and $H\curvearrowright (Y,\nu )$ are free p.m.p. actions which are Shannon orbit equivalent (that is, the cocycle partitions all have finite Shannon entropy), then the maximum sofic measure entropies of the actions satisfy

(1) $$ \begin{align} h_\nu (H\curvearrowright Y) \geq h_\mu (G\curvearrowright X). \end{align} $$

One property shared by the groups G in this theorem is that their first $\ell ^2$ -Betti number vanishes, which in the non-amenable world can be roughly intuited as an expression of anti-freeness, and indeed our approach breaks down for free groups (see [Reference Kerr and Li25, §3.5]). In what is surely not a coincidence, groups whose Bernoulli actions are cocycle superrigid also have vanishing first $\ell ^2$ -Betti number [Reference Peterson and Sinclair35], and it has been speculated that these two properties are equivalent in the non-amenable realm (curiously, however, Bernoulli cocycle or orbit equivalence superrigidity remains generally unknown for wreath products of the form ${\mathbb Z}\wr H$ with H non-amenable, which satisfy the hypotheses on G above).

Given that non-amenable products of countably infinite groups form a standard class of examples within the circle of ideas around superrigidity, cost one, and vanishing first $\ell ^2$ -Betti number, and in particular are known to satisfy Bernoulli cocycle superrigidity by a theorem of Popa [Reference Popa36], it is natural to wonder whether the entropy inequality (1) holds if G is instead assumed to be such a product. In [Reference Kerr and Li25] we demonstrated, in analogy with Gaboriau’s result on cost for products of equivalence relations [Reference Gaboriau13], that product actions of non-locally-finite product groups, when equipped with an arbitrary invariant probability measure, satisfy property SC, which is sufficient for establishing (1). However, such actions always have maximum sofic entropy zero or $-\infty $ . One of the main questions motivating the present paper is whether one can remove this product structure hypothesis on the action.

To this end we establish Theorem A below, which gives the conclusion for bounded orbit equivalence (that is, orbit equivalence with finite cocycle partitions, as explained in §2.3) and uniquely ergodic actions. We say that a p.m.p. action $G\curvearrowright (X,\mu )$ is uniquely ergodic if the only G-invariant mean on $L^\infty (X,\mu )$ is integration with respect to $\mu $ , that is, the induced action of G on the spectrum of $L^\infty (X,\mu )$ is uniquely ergodic in the usual sense of topological dynamics. When $\mu $ is atomless, unique ergodicity forces the acting group to be non-amenable [Reference Schmidt39, Theorem 2.4]. In fact an ergodic p.m.p. action $G\curvearrowright (X,\mu )$ is uniquely ergodic if and only if the restriction of the Koopman representation to $L^2 (X,\mu )\ominus {\mathbb C} 1$ does not weakly contain the trivial representation [Reference Schmidt39, Proposition 2.3]. It follows that if G is non-amenable then unique ergodicity holds whenever the restriction of the Koopman representation to the orthogonal complement of the constants is a direct sum of copies of the left regular representation, and in particular when the action has completely positive entropy [Reference Hayes15, Corollary 1.2][Reference Seward40, Corollary 1.7], and thus occurs in the following examples:

  1. (i) Bernoulli actions $G\curvearrowright (X^G ,\mu ^G )$ , where $(X,\mu )$ is a standard probability space and $(gx)_h = x_{g^{-1}h}$ for all $g,h\in G$ and $x\in X^G$ (see [Reference Kerr and Li24, §2.3.1]);

  2. (ii) algebraic actions of the form $G\curvearrowright (\widehat {({\mathbb Z} G)^n / ({\mathbb Z} G)^n A} ,\mu )$ where $A\in M_n ({\mathbb Z} G)$ is invertible as an operator on $\ell ^2 (G)^{\oplus n}$ and $\mu $ is the normalized Haar measure [Reference Hayes16, Corollary 1.5].

Moreover, if G has property (T) then all of its ergodic p.m.p. actions are uniquely ergodic [Reference Schmidt39, Theorem 2.5].

As above, $h_\mu (\cdot )$ denotes the maximum sofic measure entropy, and we write ${\underline {h}}_\mu (\cdot )$ for the infimum sofic measure entropy (see §2.6).

Theorem A. Let G and $\Gamma $ be countably infinite sofic groups at least one of which is not locally finite, and let H be a countable group. Let $G\times \Gamma \curvearrowright (X,\mu )$ and $H\curvearrowright (Y,\nu )$ be free p.m.p. actions which are boundedly orbit equivalent. Suppose that the action of H is uniquely ergodic. Then

$$ \begin{align*} h_\nu (H\curvearrowright Y) \ge {\underline{h}}_\mu (G\times\Gamma\curvearrowright X). \end{align*} $$

Theorem A is a direct consequence of Theorem 5.2 and Proposition 3.15. When combined with Theorem A of [Reference Kerr and Li25] it yields the following Theorem B. We say that an action is entropy regular if its maximum and infimum sofic entropies are equal, that is, the sofic entropy does not depend on the choice of sofic approximation sequence. Entropy regularity for a p.m.p. action is known to hold in the following situations:

  1. (i) the group is amenable, in which case the sofic measure entropy is equal to the amenable measure entropy [Reference Bowen6, Reference Kerr and Li23];

  2. (ii) the action is Bernoulli [Reference Bowen5, Reference Kerr and Li22];

  3. (iii) the action is an algebraic action of the form $G\curvearrowright (\widehat {({\mathbb Z} G)^n / ({\mathbb Z} G)^n A} ,\mu )$ where $A\in M_n ({\mathbb Z} G)$ is injective as an operator on $\ell ^2 (G)^{\oplus n}$ and $\mu $ is the normalized Haar measure [Reference Hayes14];

  4. (iv) the action is a shift action $G\curvearrowright \{ 1,\ldots ,n\}^G$ equipped with a Gibbs measure satisfying one of various uniqueness conditions [Reference Alpeev1, Reference Alpeev2].

For the definition of w-normality see the paragraph before Theorem 3.12.

Theorem B. Let G and H be countable sofic groups each of which either

  1. (i) contains a w-normal amenable subgroup which is neither locally finite nor virtually cyclic, or

  2. (ii) is a product of two countably infinite sofic groups at least one of which is not locally finite.

Let $G\curvearrowright (X,\mu )$ and $H\curvearrowright (Y,\nu )$ be free p.m.p. actions which are uniquely ergodic and entropy regular, and suppose that they are boundedly orbit equivalent. Then

$$ \begin{align*} h_\nu (H\curvearrowright Y) = h_\mu (G\curvearrowright X). \end{align*} $$

We note that, by a theorem of Belinskaya [Reference Belinskaya4], if two ergodic p.m.p. ${\mathbb Z}$ -actions are integrably orbit equivalent, and in particular if they are boundedly orbit equivalent, then they are measure conjugate up to an automorphism of ${\mathbb Z}$ (what is referred to as ‘flip conjugacy’). On the other hand, a bounded orbit equivalence between ergodic p.m.p. ${\mathbb Z}^d$ -actions for $d\geq 2$ can scramble local asymptotic data to the point of scuttling properties like mixing and completely positive entropy, as Fieldsteel and Friedman demonstrated in [Reference Fieldsteel and Friedman12].

Our strategy for proving Theorem A is to localize property SC to sofic approximations, yielding what we call ‘property sofic SC’ for a group or an action, or more generally ‘property ${\mathscr S}$ -SC’ where ${\mathscr S}$ is a collection of sofic approximations for the group in question (see §3.1). The advantage of this localization is that the action itself need not have a product structure, only the sofic approximation used to model it. This accounts for the appearance of the infimum sofic entropy in Theorem A, in contrast to (1), but as noted above many actions of interest are known to be entropy regular, in which case one does in fact get (1). The trade-off in using property sofic SC is its natural and frustratingly stubborn compatibility with the point-map formulation of sofic entropy, which is a kind of dualization of the homomorphism picture adopted in [Reference Kerr and Li25] and requires the choice of a topological model. This has put us into the situation of not being able to control the empirical distribution of microstates except under the hypothesis of unique ergodicity, when the variational principle makes such control unnecessary for the purpose of computing the entropy, and even then we have had to restrict the hypothesis on the orbit equivalence from Shannon to bounded.

Given that we are adhering to the point-map picture with its use of topological models, it makes sense to isolate as much of the argument as possible to the purely topological framework, which also has its own independent interest. Accordingly we establish the following theorem, the second part of which goes into proving Theorem A via Theorem 5.2. It is a direct consequence of Theorems 4.1 and 3.12 and Proposition 3.15. Here $h (\cdot )$ denotes the maximum sofic topological entropy and ${\underline {h}} (\cdot )$ the infimum sofic topological entropy (see §2.5).

Theorem C. Let $G\curvearrowright X$ and $H\curvearrowright Y$ be topologically free continuous actions of countable sofic groups on compact metrizable spaces, and suppose that they are continuously orbit equivalent. If G contains a w-normal amenable subgroup which is neither locally finite nor virtually cyclic then

$$ \begin{align*} h (H\curvearrowright Y) \ge h (G\curvearrowright X), \end{align*} $$

while if G is a product of two countably infinite groups at least one of which is not locally finite then

$$ \begin{align*} h (H\curvearrowright Y) \ge {\underline{h}} (G\curvearrowright X). \end{align*} $$

If the actions of G and H above are genuinely free or if G and H are torsion-free, then, using the variational principle [Reference Kerr and Li24, Theorem 10.35] and (in the case of torsion-free G and H) the main result of [Reference Meyerovitch30], one can also derive the first part of the above theorem from Theorem A of [Reference Kerr and Li25], or from [Reference Austin3] if G and H are in addition amenable and finitely generated.

In parallel with the p.m.p. setting, we define a continuous action of a countable sofic group on a compact metrizable space to be entropy regular if its maximum and infimum sofic topological entropies are equal, and note that this occurs in the following situations:

  1. (i) the group is amenable, in which case the sofic topological entropy is equal to the amenable topological entropy [Reference Kerr and Li23];

  2. (ii) the action is a shift action $G\curvearrowright X^G$ where X is a compact metrizable space [Reference Kerr and Li24, Proposition 10.28];

  3. (iii) the action is an algebraic action of the form $G\curvearrowright \widehat {({\mathbb Z} G)^n / ({\mathbb Z} G)^n A}$ where $A\in M_n ({\mathbb Z} G)$ is injective as an operator on $\ell ^2 (G)^{\oplus n}$ [Reference Hayes14].

From Theorem C we immediately obtain the following result.

Theorem D. Let G and H be countable sofic groups each of which either

  1. (a) contains a w-normal amenable subgroup which is neither locally finite nor virtually cyclic, or

  2. (b) is a product of two countably infinite sofic groups at least one of which is not locally finite.

Let $G\curvearrowright X$ and $H\curvearrowright Y$ be topologically free and entropy regular continuous actions on compact metrizable spaces, and suppose that they are continuously orbit equivalent. Then

$$ \begin{align*} h(H\curvearrowright Y) = h(G\curvearrowright X). \end{align*} $$

It was shown in [Reference Chung and Jiang7, Reference Cohen8] that the finite-base shift actions of a finitely generated group satisfy continuous cocycle superrigidity if and only if the group has one end (a property that the groups in Theorem D possess when they are finitely generated—see [Reference Chung and Jiang7, Example 1]). As observed in [Reference Chung and Jiang7], this implies, in conjunction with a theorem from [Reference Li28], that if a finitely generated group is torsion-free and amenable then each of its shift actions with finite base is continuous orbit equivalence superrigid. Whether such superrigidity ever occurs in the non-amenable setting appears, however, to be unknown.

We begin the main body of the paper in §2 by setting up general notation and reviewing terminology concerning continuous and bounded orbit equivalence and sofic entropy. In §3.1 we define properties ${\mathscr S}$ -SC and sofic SC for groups, p.m.p. actions, and continuous actions on compact metrizable spaces. In §3.2 we determine that a countable group fails to have property sofic SC if it is locally finite or finitely generated and virtually free. In §3.3 we verify that, for free p.m.p. actions, property SC implies property sofic SC, and then use this in conjunction with [Reference Kerr and Li25] to show that (i) for countable amenable groups property sofic SC is equivalent to the group being neither locally finite nor virtually cyclic, and (ii) if a countable group has a w-normal subgroup which is amenable but neither locally finite nor virtually cyclic then the group has property sofic SC. In §3.4 we prove that if a w-normal subgroup has property sofic SC then so does the ambient group, while in §3.5 we determine that the product of two countably infinite groups has property ${\mathscr S}$ -SC, where ${\mathscr S}$ is the collection of product sofic approximations, if and only if at least one of the factors is not locally finite. §§3.6 and 3.7 show property sofic SC to be an invariant of continuous orbit equivalence for topologically free continuous actions on compact metrizable spaces and of bounded orbit equivalence for free p.m.p. actions. Section 4 is devoted to the proof of Theorem 4.1, which together with Theorem 3.12 and Proposition 3.15 gives Theorem C. Finally, in §5 we establish Theorem 5.2, which together with Proposition 3.15 yields Theorem A.

2 Preliminaries

2.1 Basic notation and terminology

Throughout the paper G and H are countable discrete groups, with identity elements $e_G$ and $e_H$ . We write ${\mathcal F}(G)$ for the collection of all non-empty finite subsets of G, and $\overline {{\mathcal F}}(G)$ for the collection of symmetric finite subsets of G containing $e_G$ . For a non-empty finite set V, the algebra of all subsets of V is denoted by ${\mathbb P}_V\!,$ the group of all permutations of V by $\operatorname {\mathrm {Sym}} (V)$ , and the uniform probability measure on V by $\mathrm {m}$ .

Given a property P, a group is said to be virtually P if it has a subgroup of finite index with property P, and locally P if each of its finitely generated subgroups has property P.

A standard probability space is a standard Borel space (that is, a Polish space with its Borel $\sigma $ -algebra) equipped with a probability measure. Partitions of such a space are always understood to be Borel. A p.m.p. (probability-measure preserving) action of G is an action $G\curvearrowright (X,\mu )$ of G on a standard probability space by measure-preserving transformations. Such an action is free if the set $X_0$ of all $x\in X$ such that $sx \neq x$ for all $s\in G\setminus \{ e_G \}$ has measure one. Two p.m.p. actions $G\curvearrowright (X,\mu )$ and $G\curvearrowright (Y,\nu )$ are measure conjugate if there exist G-invariant conull sets $X_0\subseteq X$ and $Y_0\subseteq Y$ and a G-equivariant measure isomorphism $X_0 \to Y_0$ .

A continuous action $G\curvearrowright X$ on a compact metrizable space is said to be topologically free if the $G_\delta $ set of all $x\in X$ such that $sx \neq x$ for all $s\in G\setminus \{ e_G \}$ is dense. It is uniquely ergodic if there is a unique G-invariant Borel probability measure on X. By the Riesz representation theorem this is equivalent to the existence of a unique G-invariant state (that is, unital positive linear functional) for the induced action of G on the C $^*$ -algebra $C(X)$ of continuous functions on X given by $(gf)(x) = f(g^{-1} x)$ for all $g\in G$ , $f\in C(X)$ , and $x\in X$ .

A p.m.p. action $G\curvearrowright (X,\mu )$ is uniquely ergodic if there is a unique state (or mean as it is also called in this setting) on $L^\infty (X,\mu )$ which is invariant for the action of G given by $(gf)(x) = f(g^{-1} x)$ for all $g\in G$ , $f\in L^\infty (X,\mu )$ , and $x\in X$ . By Gelfand theory, this is equivalent to the unique ergodicity, in the topological-dynamical sense above, of the induced action of G on the spectrum of $L^\infty (X,\mu )$ .

2.2 Continuous orbit equivalence

We say that two continuous actions $G\curvearrowright X$ and $H\curvearrowright Y$ on compact metrizable spaces are continuously orbit equivalent if there exist a homeomorphism $\Phi : X\to Y$ and continuous maps $\kappa : G\times X \to H$ and $\lambda : H\times Y \to G$ such that

$$ \begin{align*} \Phi (gx) &= \kappa (g,x) \Phi (x) ,\\ \Phi^{-1} (ty) &= \lambda (t,y) \Phi^{-1} (y) \end{align*} $$

for all $g\in G$ , $x\in X$ , $t\in H$ , and $y\in Y$ . Such a $\Phi $ is called a continuous orbit equivalence.

If the action $H\curvearrowright Y$ is topologically free then the continuity of $\Phi $ implies that the map $\kappa $ is uniquely determined by the first line of the above display and satisfies the cocycle identity

$$ \begin{align*} \kappa (fg,x) = \kappa (f,gx) \kappa (g,x) \end{align*} $$

for $f,g\in G$ and $x\in X$ . In the case that both $G\curvearrowright X$ and $H\curvearrowright Y$ are topologically free we have

$$ \begin{align*} \lambda (\kappa (g,x),\Phi (x)) = g \end{align*} $$

for all $g\in G$ and $x\in X$ , and $\lambda $ is uniquely determined by this identity.

2.3 Bounded orbit equivalence

Two free p.m.p. actions $G\curvearrowright (X,\mu )$ and $H\curvearrowright (Y,\nu )$ are orbit equivalent if there exist a G-invariant conull set $X_0 \subseteq X$ , an H-invariant conull set $Y_0 \subseteq Y$ , and a measure isomorphism $\Psi : X_0 \to Y_0$ such that $\Psi (Gx) = H\Psi (x)$ for all $x\in X_0$ . Such a $\Psi $ is called an orbit equivalence. Associated to $\Psi $ are the cocycles $\kappa : G\times X_0 \to H$ and $\lambda : H\times Y_0 \to G$ determined (up to null sets, in accord with our definition of freeness) by

$$ \begin{align*} \Psi (gx) &= \kappa (g,x)\Psi (x) , \\ \Psi^{-1} (ty) &= \lambda (t,y) \Psi^{-1} (y) \end{align*} $$

for all $g\in G$ , $x\in X_0$ , $t\in H$ , and $y\in Y_0$ . We say that the cocycle $\kappa $ is bounded if $\kappa (g,X_0 )$ is finite for every $g\in G$ , and define boundedness for $\lambda $ likewise. If $X_0$ , $Y_0$ , and $\Psi $ can be chosen so that $\kappa $ and $\lambda $ are both bounded, then we say that the actions are boundedly orbit equivalent, and refer to $\Psi $ as a bounded orbit equivalence.

2.4 Sofic approximations

Given a non-empty finite set V, we define on $V^V$ the normalized Hamming distance

$$ \begin{align*} \rho_{\mathrm{Hamm}} (T,S) = \frac{1}{|V|} |\{ v\in V : Tv \neq Sv \} |. \end{align*} $$

A sofic approximation for G is a (not necessarily multiplicative) map $\sigma : G\to \operatorname {\mathrm {Sym}} (V)$ for some non-empty finite set V. Given a finite set $F\subseteq G$ and a $\delta> 0$ , we say that such a $\sigma $ is an $(F,\delta )$ -approximation if

  1. (i) $\rho _{\mathrm {Hamm}} (\sigma _{st} , \sigma _s \sigma _t ) \leq \delta $ for all $s,t\in F$ , and

  2. (ii) $\rho _{\mathrm {Hamm}} (\sigma _s , \sigma _t ) \geq 1-\delta $ for all distinct $s,t\in F$ .

A sofic approximation sequence for G is a sequence $\Sigma = \{ \sigma _k : G\to \operatorname {\mathrm {Sym}} (V_k ) \}_{k=1}^\infty $ of sofic approximations for G such that for every finite set $F\subseteq G$ and $\delta> 0$ there exists a $k_0 \in {\mathbb N}$ such that $\sigma _k$ is an $(F,\delta )$ -approximation for every $k\geq k_0$ . A sofic approximation $\sigma : G\to \operatorname {\mathrm {Sym}} (V)$ is said to be good enough if it is an $(F,\delta )$ -approximation for some finite set $F\subseteq G$ and $\delta> 0$ and this condition is sufficient for the purpose at hand.

The group G is sofic if it admits a sofic approximation sequence, which is the case for instance if G is amenable or residually finite. It is not known whether non-sofic groups exist.

Given a sofic approximation $\sigma : G\to \operatorname {\mathrm {Sym}} (V)$ and a set $A\subseteq G$ , we define an A-path to be a finite tuple $(v_0 , v_1 , \ldots , v_n )$ of points in V such that for every $i=1,\ldots , n$ there is a $g\in A$ for which $v_i = \sigma _g v_{i-1}$ . The integer n is the length of the path, the points $v_0 , \ldots , v_n$ its vertices, and $v_0$ and $v_n$ its endpoints. When $n=1$ we also speak of an A-edge. For $r\in {\mathbb N}$ , we say that a set $W\subseteq V$ is $(A,r)$ -separated if $\sigma _{A^r} v \cap \sigma _{A^r} w = \emptyset $ for all distinct $v,w\in W$ .

2.5 Sofic topological entropy

Let $G\curvearrowright X$ be a continuous action on a compact metrizable space. Let d be a compatible metric on X. Let F be a finite subset of G and $\delta> 0$ . Let $\sigma : G\to \operatorname {\mathrm {Sym}} (V)$ be a sofic approximation for G. On the set of maps $V \to X$ define the pseudometrics

$$ \begin{align*} d_2 (\varphi ,\psi ) &= \bigg( \frac{1}{|V|} \sum_{v\in V} d(\varphi (v),\psi (v))^2 \bigg)^{1/2} , \\d_\infty (\varphi ,\psi ) &= \max_{v\in V} d(\varphi (v),\psi (v)). \end{align*} $$

Define $\operatorname {\mathrm {Map}}_d (F,\delta ,\sigma )$ to be the set of all maps $\varphi : V\to X$ such that $d_2 (\varphi \sigma _g,g\varphi ) \leq \delta $ for all $g\in F$ . For a pseudometric space $(\Omega ,\rho )$ and $\varepsilon> 0$ we write $N_\varepsilon (\Omega ,\rho )$ for the maximum cardinality of a subset $\Omega _0$ of $\Omega $ which is $(\rho ,\varepsilon )$ -separated in the sense that $\rho (\omega _1 ,\omega _2 ) \geq \varepsilon $ for all distinct $\omega _1 ,\omega _2 \in \Omega _0$ .

Let $\Sigma = \{ \sigma _k : G\to \operatorname {\mathrm {Sym}} (V_k ) \}_{k=1}^\infty $ be a sofic approximation sequence for G. For $\varepsilon> 0$ we set

$$ \begin{align*} h_{\Sigma ,\infty}^\varepsilon (G\curvearrowright X) &= \inf_F \inf_{\delta> 0} \limsup_{k\to\infty} \frac{1}{|V_k|} \log N_\varepsilon (\operatorname{\mathrm{Map}}_d (F,\delta ,\sigma_k ) , d_\infty ) ,\\ h_{\Sigma ,2}^\varepsilon (G\curvearrowright X) &= \inf_F \inf_{\delta > 0} \limsup_{k\to\infty} \frac{1}{|V_k|} \log N_\varepsilon (\operatorname{\mathrm{Map}}_d (F,\delta ,\sigma_k ) , d_2 ) , \end{align*} $$

where the first infimum in each case is over all finite sets $F\subseteq G$ . The sofic topological entropy of the action $G\curvearrowright X$ with respect to $\Sigma $ is then defined by

$$ \begin{align*} h_{\Sigma} (G{\curvearrowright} X) = \sup_{\varepsilon> 0} h_{\Sigma ,\infty}^{\varepsilon} (G\curvearrowright X). \end{align*} $$

This quantity does not depend on the choice of compatible metric d, as is readily seen, and by [Reference Kerr and Li24, Proposition 10.23] we can also compute it using separation with respect to $d_2$ , that is,

$$ \begin{align*} h_\Sigma (G\curvearrowright X) = \sup_{\varepsilon> 0} h_{\Sigma ,2}^\varepsilon (G\curvearrowright X). \end{align*} $$

We define the maximum and infimum sofic topological entropies of $G\curvearrowright X$ by

$$ \begin{align*} h (G\curvearrowright X) &= \max_\Sigma h_\Sigma (G\curvearrowright X) ,\\ {\underline{h}} (G\curvearrowright X) &= \inf_\Sigma h_\Sigma (G\curvearrowright X) , \end{align*} $$

where $\Sigma $ ranges in each case over all sofic approximation sequences for G (when G is non-sofic we interpret these quantities to be $-\infty $ ). It is a straightforward exercise to show that the maximum does indeed exist (we do not know, however, whether the infimum is always realized). Note that $-\infty $ is a possible value for $h_\Sigma (G\curvearrowright X)$ , and so if it occurs for some $\Sigma $ then ${\underline {h}} (G\curvearrowright X) = -\infty $ , and if it occurs for all $\Sigma $ then $h (G\curvearrowright X) = -\infty $ . The action $G\curvearrowright X$ is entropy regular if its maximum and infimum sofic topological entropies are equal, that is, the sofic topological entropy does not depend on the choice of sofic approximation sequence.

2.6 Sofic measure entropy

Let $G\curvearrowright (X,\mu )$ be a p.m.p. action. Let ${\mathscr C}$ be a finite Borel partition of X, F a finite subset of G containing $e_G$ , and $\delta> 0$ . Write $\mathrm {alg} ({\mathscr C} )$ for the algebra generated by ${\mathscr C}$ , which consists of all unions of members of ${\mathscr C}$ , and write ${\mathscr C}_F$ for the join $\bigvee _{s\in F} s{\mathscr C}$ . Let $\sigma : G\to \operatorname {\mathrm {Sym}}(V)$ be a sofic approximation for G. Write $\operatorname {\mathrm {Hom}}_\mu ({\mathscr C} ,F,\delta ,\sigma )$ for the set of all homomorphisms $\varphi : \mathrm {alg} ({\mathscr C}_F )\to {\mathbb P}_V$ satisfying

  1. (i) $\sum _{A\in {\mathscr C}} \mathrm {m} (\sigma _g \varphi (A) \Delta \varphi (gA)) < \delta $ for all $g\in F$ , and

  2. (ii) $\sum _{A\in {\mathscr C}_F} |\mathrm {m} (\varphi (A)) - \mu (A)| < \delta $ .

For a finite Borel partition ${\mathscr P}\leq {\mathscr C}$ we write $\lvert \operatorname {\mathrm {Hom}}_\mu ({\mathscr C} ,F,\delta ,\sigma )\rvert _{\mathscr P}$ for the cardinality of the set of restrictions of elements of $\operatorname {\mathrm {Hom}}_\mu ({\mathscr C} ,F,\delta ,\sigma )$ to ${\mathscr P}$ .

Given a sofic approximation sequence $\Sigma = \{ \sigma _k : G\to \operatorname {\mathrm {Sym}} (V_k ) \}_{k=1}^\infty $ for G, we define the sofic measure entropy of the action $G\curvearrowright (X,\mu )$ with respect to $\Sigma $ by

$$ \begin{align*} h_{\Sigma ,\mu} (G\curvearrowright X) = \sup_{\mathscr P} \inf_{{\mathscr C}\geq{\mathscr P}} \inf_F \inf_{\delta> 0} \limsup_{k\to\infty} \frac{1}{|V_k|} \log\ \lvert\operatorname{\mathrm{Hom}}_\mu ({\mathscr C} ,F,\delta ,\sigma_k )\rvert_{\mathscr P} , \end{align*} $$

where the supremum is over all finite partitions ${\mathscr P}$ of X, the first infimum is over all finite partitions ${\mathscr C}$ of X refining ${\mathscr P}$ , and the second infimum is over all finite sets $F\subseteq G$ containing $e_G$ .

As in the topological case, one can check that there is a maximum among the quantities $h_{\Sigma ,\mu } (G\curvearrowright X)$ over all sofic approximation sequences $\Sigma $ for G, where $-\infty $ is included as a possible value. The maximum and infimum sofic measure entropies of $G\curvearrowright (X,\mu )$ are then defined by

$$ \begin{align*} h_\mu (G\curvearrowright X) &= \max_\Sigma h_{\Sigma ,\mu} (G\curvearrowright X) , \\ {\underline{h}}_\mu (G\curvearrowright X) &= \inf_\Sigma h_{\Sigma ,\mu} (G\curvearrowright X) , \end{align*} $$

where $\Sigma $ ranges in each case over all sofic approximation sequences for G. When G is non-sofic these quantities are interpreted to be $-\infty $ . The action is entropy regular if its maximum and infimum sofic measure entropies are equal, that is, the sofic measure entropy does not depend on the choice of sofic approximation sequence.

3 Properties ${\mathscr S}$ -SC and sofic SC

3.1 Definitions of properties ${\mathscr S}$ -SC and sofic SC

Write ${\mathscr S}_G$ for the collection of all sofic approximations for G. Let ${\mathscr S}$ be any collection of sofic approximations for G.

Definition 3.1. We say that the group G has property ${\mathscr S}$ -SC (or property sofic SC if ${\mathscr S} = {\mathscr S}_G$ ) if for any function $\Upsilon : {\mathcal F}(G)\rightarrow [0, \infty )$ there exists an $S\in \overline {{\mathcal F}}(G)$ such that for any $T\in \overline {{\mathcal F}}(G)$ there are $C, n\in {\mathbb N}$ , and $S_1, \ldots , S_n\in \overline {{\mathcal F}}(G)$ such that for every good enough sofic approximation $\pi : G\rightarrow \operatorname {\mathrm {Sym}}(V)$ in ${\mathscr S}$ there are subsets W and ${\mathcal V}_j$ of V for $1\le j\le n$ satisfying the following conditions:

  1. (i) $\sum _{j=1}^n \Upsilon (S_j)\mathrm {m}({\mathcal V}_j)\le 1$ ;

  2. (ii) $\bigcup _{g\in S}\pi _gW=V$ ;

  3. (iii) if $w_1, w_2\in W$ satisfy $\pi _gw_1=w_2$ for some $g\in T$ then $w_1$ and $w_2$ are connected by a path of length at most C in which each edge is of the form $(v, \pi _hv)$ for some $1\le j\le n$ , $h\in S_j$ , and $v\in {\mathcal V}_j$ with $\pi _hv\in {\mathcal V}_j$ .

Definition 3.2. We say that a continuous action $G\curvearrowright X$ on a compact metrizable space X with compatible metric d has property ${\mathscr S}$ -SC (or property sofic SC if ${\mathscr S} = {\mathscr S}_G$ ) if for any function $\Upsilon : {\mathcal F}(G)\rightarrow [0, \infty )$ there exists an $S\in \overline {{\mathcal F}}(G)$ such that for any $T\in \overline {{\mathcal F}}(G)$ there are $C, n\in {\mathbb N}$ , $S_1, \ldots , S_n\in \overline {{\mathcal F}}(G)$ , $F^\sharp \in {\mathcal F}(G)$ , and $\delta ^\sharp>0$ such that for every good enough sofic approximation $\pi : G\rightarrow \operatorname {\mathrm {Sym}}(V)$ in ${\mathscr S}$ with $\operatorname {\mathrm {Map}}_d(F^\sharp , \delta ^\sharp , \pi )\neq \emptyset $ there are W and ${\mathcal V}_j$ for $1\le j\le n$ as in Definition 3.1. By [Reference Kerr and Li24, Lemma 10.24] this does not depend on the choice of d.

Definition 3.3. We say that a p.m.p. action $G\curvearrowright (X,\mu )$ has property ${\mathscr S}$ -SC (or property sofic SC if ${\mathscr S} = {\mathscr S}_G$ ) if for any function $\Upsilon : {\mathcal F}(G)\rightarrow [0, \infty )$ there exists an $S\in \overline {{\mathcal F}}(G)$ such that for any $T\in \overline {{\mathcal F}}(G)$ there are $C, n\in {\mathbb N}$ , $S_1, \ldots , S_n\in \overline {{\mathcal F}}(G)$ , a finite Borel partition ${\mathscr C\,}^\sharp $ of X, an $F^\sharp \in {\mathcal F}(G)$ containing $e_G$ , and a $\delta ^\sharp>0$ such that for every good enough sofic approximation $\pi : G\rightarrow \operatorname {\mathrm {Sym}}(V)$ in ${\mathscr S}$ with $\operatorname {\mathrm {Hom}}_\mu ({\mathscr C\,}^\sharp , F^\sharp , \delta ^\sharp , \pi )\neq \emptyset $ there are W and ${\mathcal V}_j$ for $1\le j\le n$ as in Definition 3.1.

The following proposition shows that, when G is finitely generated, in Definition 3.1 we can fix $n=1$ and take $S_1$ to be any symmetric finite generating subset of G containing $e_G$ , but with the price that $\bigcup _{g\in S} \pi _g W$ is only most of V instead of the whole of V.

Proposition 3.4. Suppose that G is finitely generated. Let A be a generating set for G in $\overline {{\mathcal F}}(G)$ . Then G has property ${\mathscr S}$ -SC if and only if for any $\varepsilon>0$ there exists an $S\in \overline {{\mathcal F}}(G)$ such that for any $T\in \overline {{\mathcal F}}(G)$ and $\delta>0$ there is a $C\in {\mathbb N}$ such that for any good enough sofic approximation $\pi : G\rightarrow \operatorname {\mathrm {Sym}}(V)$ in ${\mathscr S}$ there are subsets W and ${\mathcal V}$ of V satisfying the following conditions:

  1. (i) $\mathrm {m}({\mathcal V})\le \varepsilon $ ;

  2. (ii) $\mathrm {m}(\bigcup _{g\in S}\pi _gW)\ge 1-\delta $ ;

  3. (iii) if $w_1, w_2\in W$ satisfy $\pi _gw_1=w_2$ for some $g\in T$ then $w_1$ and $w_2$ are connected by an A-path of length at most C whose vertices all lie in ${\mathcal V}$ .

Proof. Denote by $\ell _A$ the word length function on G associated to A.

Suppose first that G has property ${\mathscr S}$ -SC. Let $\varepsilon>0$ . Define $\Upsilon : {\mathcal F}(G)\rightarrow [0, \infty )$ by $\Upsilon (F)=\varepsilon ^{-1}|A|^{\max _{g\in F}\ell _A(g)}$ . Then there is an $S\in \overline {{\mathcal F}}(G)$ witnessing property ${\mathscr S}$ -SC. Let $T\in \overline {{\mathcal F}}(G)$ and $\delta>0$ . Then we have $C, n, S_1, \ldots , S_n$ as given by Definition 3.1. Set $m=\max _{1\le j\le n}\max _{g\in S_j}\ell _A(g)$ . Let $\pi : G\rightarrow \operatorname {\mathrm {Sym}}(V)$ be a good enough sofic approximation for G in ${\mathscr S}$ . Then we have W and ${\mathcal V}_1, \ldots , {\mathcal V}_n$ satisfying conditions (i)–(iii) in Definition 3.1. Denote by $V'$ the set of all $v\in V$ satisfying $\pi _{gh}v=\pi _g\pi _h v$ for all $g, h\in A^{mC}$ . When $\pi $ is a good enough sofic approximation, we have $\mathrm {m}(V\setminus V')\le \delta /|S|$ . Set $W'=W\cap V'$ . For each $1\le j\le n$ , set $m_j=\max _{g\in S_j}\ell _A(g)$ and ${\mathcal V}_j^\dagger =\bigcup _{g\in A^{m_j}}\pi _g{\mathcal V}_j$ . Set ${\mathcal V}=\bigcup _{j=1}^n{\mathcal V}_j^\dagger $ . Then

$$ \begin{align*} \mathrm{m}({\mathcal V})\le \sum_{j=1}^n\mathrm{m}({\mathcal V}_j^\dagger)\le \sum_{j=1}^n|A^{m_j}|\cdot \mathrm{m}({\mathcal V}_j)\le \varepsilon\sum_{j=1}^n\Upsilon(S_j)\mathrm{m}({\mathcal V}_j)\le \varepsilon, \end{align*} $$

verifying condition (i) in the proposition statement. Note also that

$$ \begin{align*}\mathrm{m}\bigg(\bigcup_{g\in S}\pi_gW'\bigg)\ge \mathrm{m}\bigg(\bigcup_{g\in S}\pi_g W\bigg)-|S|\cdot \mathrm{m}(V\setminus V')\ge 1-\delta,\end{align*} $$

which verifies condition (ii) in the proposition statement. Let $g\in T$ and $w_1, w_2\in W'$ be such that $\pi _g w_1=w_2$ . Then $w_1$ and $w_2$ are connected by a path of length at most C in which each edge is an $S_j$ -edge with both endpoints in ${\mathcal V}_j$ for some $1\le j\le n$ . It is easily checked that the endpoints of such an edge are connected by an A-path of length at most $m_j$ with all vertices in ${\mathcal V}_j^\dagger $ . Thus $w_1$ and $w_2$ are connected by an A-path of length at most $Cm$ with all vertices in ${\mathcal V}$ , verifying condition (iii) in the proposition statement. This proves the ‘only if’ part.

To prove the ‘if’ part, suppose that G satisfies the condition in the statement of the proposition. Let $\Upsilon $ be a function ${\mathcal F}(G)\rightarrow [0, \infty )$ . Take $0<\varepsilon <1/(2\Upsilon (A))$ . Then we have an S as in the statement of the proposition. Let $T\in \overline {{\mathcal F}}(G)$ . Take $0< \delta <1/(6|T|\Upsilon (T))$ . Then we have a C as in the statement of the proposition. Set $n=2$ , $S_1=A$ , and $S_2=T$ . Let $\pi : G\rightarrow \operatorname {\mathrm {Sym}}(V)$ be a good enough sofic approximation for G in ${\mathscr S}$ . Then we have W and ${\mathcal V}$ as in the statement of the proposition. Set $W'=W\cup \pi _{e_G}^{-1}(V\setminus \bigcup _{g\in S}\pi _g W)$ . Then $\bigcup _{g\in S}\pi _gW'=V$ , verifying condition (ii) in Definition 3.1. Set ${\mathcal V}_1={\mathcal V}$ and ${\mathcal V}_2=\bigcup _{g\in T}((W'\setminus W)\cup \pi _g(W'\setminus W)\cup \pi _g^{-1}(W'\setminus W))$ . Then

$$ \begin{align*} \mathrm{m}({\mathcal V}_2)\le (2|T|+1)\mathrm{m}(W'\setminus W)\le 3|T|\delta, \end{align*} $$

and hence

$$ \begin{align*} \Upsilon(S_1)\mathrm{m}({\mathcal V}_1)+\Upsilon(S_2)\mathrm{m}({\mathcal V}_2)\le \Upsilon(A)\varepsilon+3\Upsilon(T)|T|\delta< \tfrac12 + \tfrac12 = 1, \end{align*} $$

which verifies condition (i) in Definition 3.1. Let $g\in T$ and $w_1, w_2\in W'$ be such that $\pi _gw_1=w_2$ . If $w_1\not \in W$ or $w_2\not \in W$ , then $(w_1, w_2)$ is an $S_2$ -edge with both endpoints in ${\mathcal V}_2$ . If $w_1, w_2\in W$ , then $w_1$ and $w_2$ are connected by an $S_1$ -path of length at most C such that all vertices of this path lie in ${\mathcal V}={\mathcal V}_1$ , yielding condition (iii) in Definition 3.1.

3.2 Groups without property sofic SC

Let ${\mathscr S}\,$ be a collection of sofic approximations for G which contains arbitrarily good sofic approximations (or, equivalently, which contains a sofic approximation sequence). In Propositions 3.6 and 3.7 we identify two classes of groups which fail to have property ${\mathscr S}$ -SC, and in particular fail to have property sofic SC.

Lemma 3.5. Suppose that G is finite. Then G does not have property ${\mathscr S}$ -SC.

Proof. Suppose to the contrary that G has property ${\mathscr S}$ -SC. Define $\Upsilon : {\mathcal F}(G)\rightarrow [0, \infty )$ by $\Upsilon (F)=4|G|$ for all $F\in {\mathcal F}(G)$ . Then there is some $S\in \overline {{\mathcal F}}(G)$ satisfying the conditions in Definition 3.1. Put $T=\{e_G\}$ . Then there are $C, n\in {\mathbb N}$ and $S_1, \ldots , S_n\in \overline {{\mathcal F}}(G)$ satisfying the conditions in Definition 3.1.

Let $\pi : G\rightarrow \operatorname {\mathrm {Sym}}(V)$ be a good enough sofic approximation in ${\mathscr S}$ so that there are subsets W and ${\mathcal V}_1, \ldots , {\mathcal V}_n$ of V satisfying conditions (i)–(iii) in Definition 3.1 and also so that $\mathrm {m}(U)\le 1/(4|G|)$ where U consists of all $v\in V$ satisfying $\pi _{e_G}v\neq v$ . Seeing that $W\subseteq U\cup \bigcup _{j=1}^n{\mathcal V}_j$ , we have

$$ \begin{align*} \mathrm{m}(W)&\le \mathrm{m}(U)+\mathrm{m}\bigg(\bigcup_{j=1}^n{\mathcal V}_j\bigg)\le \frac{1}{4|G|}+\sum_{j=1}^n\mathrm{m}({\mathcal V}_j)\\&=\frac{1}{4|G|}+\frac{1}{4|G|}\sum_{j=1}^n\Upsilon(S_j)\mathrm{m}({\mathcal V}_j)\le \frac{1}{2|G|}. \end{align*} $$

Thus

$$ \begin{align*} 1= \mathrm{m}\bigg(\bigcup_{g\in S}\pi_gW\bigg)\le |S|\mathrm{m}(W)\le |G|\mathrm{m}(W)\le \frac12 ,\end{align*} $$

a contradiction.

Proposition 3.6. Suppose that G is locally finite. Then G does not have property ${\mathscr S}$ -SC.

Proof. Suppose to the contrary that G has property ${\mathscr S}$ -SC. Then G must be infinite by Lemma 3.5. Take a strictly increasing sequence $\{G_k\}$ of finite subgroups of G such that $G=\bigcup _{k\in {\mathbb N}}G_k$ . For each $F\in {\mathcal F}(G)$ , denote by $\Phi (F)$ the smallest $k\in {\mathbb N}$ satisfying $F\subseteq G_k$ . Define $\Upsilon : {\mathcal F}(G)\rightarrow [0, \infty )$ by $\Upsilon (F)=3|G_{\Phi (F)}|$ . Then there is some $S\in \overline {{\mathcal F}}(G)$ satisfying the conditions in Definition 3.1. Put $m=\Phi (S)$ and $T=G_{m+1}\in \overline {{\mathcal F}}(G)$ . Then there are $C, n\in {\mathbb N}$ and $S_1, \ldots , S_n\in \overline {{\mathcal F}}(G)$ satisfying the conditions in Definition 3.1. Put $M=\max \{\max _{1\le j\le n}\Phi (S_j), m+1\}$ .

Let $\pi : G\rightarrow \operatorname {\mathrm {Sym}}(V)$ be a good enough sofic approximation in ${\mathscr S}$ so that there is a set $V_1\subseteq V$ satisfying the following conditions:

  1. (i) $\pi _g\pi _hv=\pi _{gh}v$ for all $g, h\in G_M$ and $v\in V_1$ ;

  2. (ii) $\pi _gv\neq \pi _hv$ for all $v\in V_1$ and distinct $g, h\in G_M$ ;

  3. (iii) $\pi _gV_1=V_1$ for all $g\in G_M$ ;

  4. (iv) $\mathrm {m}(V_1)\ge 1/2$ .

Then $G_M$ acts on $V_1$ via $\pi $ . Denote by ${\mathscr P}$ the partition of $V_1$ into $G_{m+1}$ -orbits.

By assumption, when $\pi $ is a good enough sofic approximation we can find subsets W and ${\mathcal V}_1, \ldots , {\mathcal V}_n$ of V satisfying conditions (i)–(iii) in Definition 3.1. Note that $V=\bigcup _{g\in S}\pi _gW=\bigcup _{g\in G_m}\pi _gW$ , which implies that for every member P of ${\mathscr P}$ the intersection $P\cap W$ is not contained in a single $G_m$ -orbit.

Set ${\mathcal V}=\bigcup _{j=1}^n\pi _{G_{\Phi (S_j)}}({\mathcal V}_j\cap V_1)$ . Then

(2) $$ \begin{align} \mathrm{m}({\mathcal V})\le \!\sum_{1\le j\le n}\kern-1pt|G_{\Phi(S_j)}|\mathrm{m}({\mathcal V}_j\cap V_1)\le \!\sum_{1\le j\le n}\kern-2.5pt|G_{\Phi(S_j)}|\mathrm{m}({\mathcal V}_j)= \frac{1}{3}\!\sum_{1\le j\le n}\kern-2pt\Upsilon(S_j)\mathrm{m}({\mathcal V}_j) \kern-1pt\le\kern-1pt \frac{1}{3}. \end{align} $$

Now let $P\in {\mathscr P}$ and $w_1\in P\cap W$ . Then we can find some $w_2\in P\cap W$ such that $w_1$ and $w_2$ are in different $G_m$ -orbits. We have $w_2=\pi _tw_1$ for some $t\in G_{m+1}\setminus G_m= T\setminus G_m$ . Thus we can find some $1\le l\le C$ , $1\le j_1, \ldots , j_l\le n$ , $v_k\in {\mathcal V}_{j_k}$ for $1\le k\le l$ , and $g_k\in S_{j_k}$ for $1\le k\le l$ such that, setting $v_0=w_1$ , we have $\pi _{g_k}v_{k-1}=v_k$ for all $1\le k\le l$ and $v_l=w_2$ . Then

$$ \begin{align*} w_2=v_l=\pi_{g_l}\cdots \pi_{g_1}v_0=\pi_{g_l\cdots g_1}w_1, \end{align*} $$

and hence $g_l\cdots g_1=t$ . It follows that the elements $g_1, \ldots , g_l$ cannot all lie in $G_m$ . Denote by i the smallest k satisfying $g_k\not \in G_m$ . Then $v_i\in \pi _{G_{\Phi (S_{j_i})}}w_1$ , and hence $w_1\in \pi _{G_{\Phi (S_{j_i})}}v_i$ . Consequently,

$$ \begin{align*} \pi_{G_m}w_1\subseteq \pi_{G_m}\pi_{G_{\Phi(S_{j_i})}}v_i=\pi_{G_{\Phi(S_{j_i})}}v_i\subseteq \pi_{G_{\Phi(S_{j_i})}}({\mathcal V}_{j_i}\cap V_1)\subseteq {\mathcal V}. \end{align*} $$

Therefore $V_1=\bigcup {\mathscr P}=\pi _{G_m}(W\cap (\bigcup {\mathscr P}))\subseteq {\mathcal V}$ , whence $ \mathrm {m}({\mathcal V})\ge \mathrm {m}(V_1)\ge 1/2$ , contradicting (2).

Proposition 3.7. Suppose that G is finitely generated and virtually free. Then G does not have property ${\mathscr S}$ -SC.

Proof. By Lemma 3.5 we may assume that G is infinite. Take a free subgroup $G_1$ of G with finite index. Then $G_1$ is non-trivial and, by Schreier’s lemma, finitely generated. Take free generators $a_1, \ldots , a_r$ for $G_1$ . Set $A=\{a_1, \ldots , a_r, a_1^{-1}, \ldots , a_r^{-1}, e_G\}$ . Denote by $\ell $ the word length function on $G_1$ associated to $a_1, \ldots , a_r, a_1^{-1}, \ldots , a_r^{-1}$ . For each $n\in {\mathbb N}$ denote by $B_n$ the set of elements g in $G_1$ satisfying $\ell (g)\le n$ . Take a subset H of G containing $e_G$ such that G is the disjoint union of the sets $hG_1$ for $h\in H$ . Set $D=H\cup A$ . For each $F\in {\mathcal F}(G)$ , denote by $\Psi (F)$ the smallest $n\in {\mathbb N}$ satisfying $F\subseteq HB_n$ , and set $F'=HB_{\Psi (F)}$ .

For any $g\in G$ and $h\in H$ we can write $gh$ uniquely as $bd$ with $b\in H$ and $d\in G_1$ , and using this factorization we set R to be the maximum value of $\ell (d)$ over all $g\in D$ and $h\in H$ . Define $\Upsilon : {\mathcal F}(G)\rightarrow [0, \infty )$ by $\Upsilon (F)=3|HB_{R}|\cdot |F'|$ .

Suppose that G has property ${\mathscr S}$ -SC. Then there is some $S\in \overline {{\mathcal F}}(G)$ satisfying the conditions in Definition 3.1. Put $m=\Psi (S)$ , $N=m+1$ , and $T=S\{a_1^{2N}, e_G, a_1^{-2N}\}S\in \overline {{\mathcal F}}(G)$ . Then there are $C, n\in {\mathbb N}$ and $S_1, \ldots , S_n\in \overline {{\mathcal F}}(G)$ satisfying the conditions in Definition 3.1. Put $C'=C\max _{1\le j\le n}(1+\Psi (S_j))\in {\mathbb N}$ and $U=((HA)^{C'}HB_{2N})\cup ((HA)^{C'}HB_{2N})^{-1}\in \overline {{\mathcal F}}(G)$ .

Let $\pi : G\rightarrow \operatorname {\mathrm {Sym}}(V)$ be a good enough sofic approximation in ${\mathscr S}$ so that there are subsets W and ${\mathcal V}_1, \ldots , {\mathcal V}_n$ of V satisfying conditions (i)–(iii) in Definition 3.1 and a set $V'\subseteq V$ satisfying the following conditions:

  1. (i) $\pi _g\pi _hv=\pi _{gh}v$ for all $g, h\in U^{10}$ and $v\in V'$ ;

  2. (ii) $\pi _gv\neq \pi _hv$ for all $v\in V'$ and distinct $g, h\in U$ ;

  3. (iii) $\mathrm {m}(V')\ge 1/2$ .

For each $1\le j\le n$ , set ${\mathcal V}_j'=\bigcup _{g\in S_j'}\pi _g{\mathcal V}_j.$ Set ${\mathcal V}=\bigcup _{j=1}^n{\mathcal V}_j'$ .

Let $v\in V'$ . We have $\pi _{a_1^{N}}v=\pi _{h_1}w_1$ and $\pi _{a_1^{-N}}v=\pi _{h_2}w_2$ for some $h_1, h_2\in S$ and $w_1, w_2\in W$ . Then

$$ \begin{align*} \pi_{h_2^{-1}a_1^{-2N}h_1}w_1=\pi_{h_2}^{-1}\pi_{a_1^{-N}}\pi_{a_1^{N}}^{-1}\pi_{h_1}w_1=\pi_{h_2}^{-1}\pi_{a_1^{-N}}v=w_2. \end{align*} $$

By assumption we can find a path from $w_1$ to $w_2$ of length at most C in which each edge is an $S_j$ -edge with both endpoints in ${\mathcal V}_j$ for some $1\le j\le n$ . Replacing each such edge by a D-path of length at most $1+\Psi (S_j)$ and with all vertices in ${\mathcal V}_j'$ , we find a D-path from $w_1$ to $w_2$ of length at most $C'$ such that all vertices are in ${\mathcal V}$ . Thus we get some $1\le l\le C'$ , $v_k\in {\mathcal V}$ for $1\le k\le l$ , and $g_k\in D$ for $1\le k\le l$ such that, setting $v_0=w_1$ , we have $\pi _{g_k}v_{k-1}=v_k$ for all $1\le k\le l$ and $v_l=w_2$ . Then

$$ \begin{align*} \pi_{h_2^{-1}a_1^{-N}}v=w_2=\pi_{g_l}\cdots \pi_{g_1}w_1=\pi_{g_l\cdots g_1h_1^{-1}a_1^{N}}v. \end{align*} $$

Since $h_2^{-1}a_1^{-N}$ and $g_l\cdots g_1h_1^{-1}a_1^{N}$ belong to U, we conclude that $h_2^{-1}a_1^{-N}=g_l\cdots g_1h_1^{-1}a_1^{N}$ . Set $t_j=g_j\cdots g_1h_1^{-1}a_1^{N}\in U$ for $0\le j\le l$ . We can write each $t_j$ uniquely as $b_jd_j$ for some $b_j\in H$ and $d_j\in G_1$ . Then we have

$$ \begin{align*} \ell(d_jd_{j-1}^{-1})\le R \end{align*} $$

for all $1\le j\le l$ . Consider the path p in $G_1$ from $d_0$ to $d_l$ defined by concatenating the geodesic from $d_{j-1}$ to $d_j$ for all $1\le j\le l$ , where we endow $G_1$ with the right invariant metric induced from $\ell $ . Note that as reduced words $d_0$ and $d_l$ end with $a_1$ and $a_1^{-1}$ , respectively. Thus p passes through $e_G$ . It follows that there is some $1\le i\le l$ with $\ell (d_{i})\le R$ . Then $t_i\in HB_{R}$ , whence

$$ \begin{align*} v=\pi_{t_i}^{-1}v_i=\pi_{t_i^{-1}}v_i\in \bigcup_{g\in (HB_{R})^{-1}}\pi_g {\mathcal V}. \end{align*} $$

Therefore $V'\subseteq \bigcup _{g\in (HB_{R})^{-1}}\pi _g {\mathcal V}$ .

Now we get

$$ \begin{align*} \frac12 \le \mathrm{m}(V') &\le \mathrm{m} \bigg(\bigcup_{g\in (HB_{R})^{-1}}\pi_g {\mathcal V} \bigg) \le |HB_{R}|\mathrm{m}({\mathcal V}) \\ &\le |HB_{R}|\sum_{j=1}^n|S_j'|\mathrm{m}({\mathcal V}_j) =\frac{1}{3}\sum_{j=1}^n\Upsilon(S_j)\mathrm{m}({\mathcal V}_j)\le \frac13 , \end{align*} $$

a contradiction.

3.3 Groups with property sofic SC

In Theorems 3.11 and 3.12 below we will identify classes of groups that have property sofic SC. This will rely on results from [Reference Kerr and Li25] that we can access via the connection to property SC established in Proposition 3.10.

Definition 3.8. Let ${\mathfrak Y}$ be a class of free p.m.p. actions of a fixed infinite G. We say that ${\mathfrak Y}$ has property SC if for any function $\Upsilon : {\mathcal F}(G)\rightarrow [0, \infty )$ there exists an $S\in \overline {{\mathcal F}}(G)$ such that for any $T\in \overline {{\mathcal F}}(G)$ there are $C, n\in {\mathbb N}$ , and $S_1, \ldots , S_n\in \overline {{\mathcal F}}(G)$ so that for any $G\curvearrowright (X, \mu )$ in ${\mathfrak Y}$ there are Borel subsets W and ${\mathcal V}_j$ of X for $1\le j\le n$ satisfying the following conditions:

  1. (i) $\sum _{j=1}^n \Upsilon (S_j)\mu ({\mathcal V}_j)\le 1$ ;

  2. (ii) $SW=X$ ;

  3. (iii) if $w_1, w_2\in W$ satisfy $gw_1=w_2$ for some $g\in T$ then $w_1$ and $w_2$ are connected by a path of length at most C in which each edge is an $S_j$ -edge with both endpoints in ${\mathcal V}_j$ for some $1\le j\le n$ .

We say that a p.m.p. action $G\curvearrowright (X, \mu )$ has property SC if the singleton class containing it has property SC. We say that G itself has property SC if the class of all free p.m.p actions $G\curvearrowright (X, \mu )$ has property SC (note that freeness implies atomlessness of the measure since G is infinite).

Remark 3.9. When ${\mathfrak Y}$ consists of either a single free p.m.p. action or all free p.m.p. actions of a fixed G, the existence of the bound C is automatic, as explained in the paragraph following [Reference Kerr and Li25, Proposition 3.5].

Proposition 3.10. Suppose that G is infinite and sofic. Let $G\curvearrowright (X, \mu )$ be a free p.m.p. action with property SC. Then the action has property sofic SC.

Proof. We may assume, by passing to a suitable G-invariant conull subset of X, that the action of G is genuinely free. Let $\Upsilon $ be a function ${\mathcal F}(G)\rightarrow [0, \infty )$ . Since $G\curvearrowright (X, \mu )$ has property SC, using the function $2\Upsilon $ we find an $S\in \overline {{\mathcal F}}(G)$ such that for any $T\in \overline {{\mathcal F}}(G)$ there are $C, n\in {\mathbb N}$ , $S_1, \ldots , S_n\in \overline {{\mathcal F}}(G)$ , and Borel subsets W and ${\mathcal V}_k$ of X for $1\le k\le n$ satisfying the following conditions:

  1. (i) $2\sum _{k=1}^n \Upsilon (S_k)\mu ({\mathcal V}_k)\le 1$ ;

  2. (ii) $SW=X$ ;

  3. (iii) if $w_1, w_2\in W$ satisfy $gw_1=w_2$ for some $g\in T$ then $w_1$ and $w_2$ are connected by a path of length at most C in which each edge is an $S_k$ -edge with both endpoints in ${\mathcal V}_k$ for some $1\le k\le n$ .

Let $T\in \overline {{\mathcal F}}(G)$ . Then we have $C, n$ , $S_k$ for $1\le k\le n$ , and W and ${\mathcal V}_k$ for $1\le k\le n$ as above. We now verify conditions (i)–(iii) in Definition 3.1 as referenced in Definition 3.3.

Let $g\in T$ . For each $x\in W\cap g^{-1}W$ , we can find $g_1, \ldots , g_l\in G$ for some $1\le l\le C$ such that $g=g_lg_{l-1}\cdots g_1$ and for each $1\le j\le l$ one has $g_j\in S_{k_j}$ and $g_{j-1}\cdots g_1x, g_jg_{j-1}\cdots g_1x\in {\mathcal V}_{k_j}$ for some $1\le k_j\le n$ . Then we can find a finite Borel partition ${\mathscr C}_g$ of $W\cap g^{-1}W$ such that

$$ \begin{align*} |{\mathscr C}_g|\le Cn^C\Big(\max_{1\le k\le n}|S_k|\Big)^C \end{align*} $$

and for each $A\in {\mathscr C}_g$ we can choose the same $l, g_1, \ldots , g_l, k_1, \ldots , k_l$ for all $x\in A$ . Then for all $1\le j\le l$ the sets $g_{j-1}\cdots g_1A$ and $g_jg_{j-1}\cdots g_1A$ are contained in ${\mathcal V}_{k_j}$ .

Denote by ${\mathscr C\,}^\sharp $ the finite partition of X generated by $W, {\mathcal V}_1, \ldots , {\mathcal V}_n$ and ${\mathscr C}_g$ for $g\in T$ . Set $F^\sharp =(T\cup S\cup \bigcup _{k=1}^nS_k)^{100C}\in {\mathcal F}(G)$ . Set $D=|T|C^2n^C(\max _{1\le k\le n}|S_k|)^C>0$ , and take $\delta>0$ with $3\delta |T|\Upsilon (T)\le 1/4$ . Take

$$ \begin{align*} 0<\delta^\sharp\le \min \bigg\{ \bigg(4\sum_{k=1}^n\Upsilon(S_k)\bigg)^{-1} , \delta/(|S|(|T|+D+2)) \bigg\}. \end{align*} $$

Let $\pi : G\rightarrow \operatorname {\mathrm {Sym}}(V)$ be a sofic approximation for G with $\operatorname {\mathrm {Hom}}_\mu ({\mathscr C\,}^\sharp , F^\sharp , \delta ^\sharp , \pi )\neq \emptyset $ which is good enough so that $\mathrm {m}(V_{F^\sharp })>1-\delta ^\sharp $ , where $V_{F^\sharp }$ denotes the set of all $v\in V$ satisfying $\pi _{gh}v=\pi _g\pi _hv$ for all $g, h\in F^\sharp $ and $\pi _gv\neq \pi _h v$ for all distinct $g, h\in F^\sharp $ . Take $\varphi \in \operatorname {\mathrm {Hom}}_\mu ({\mathscr C\,}^\sharp , F^\sharp , \delta ^\sharp , \pi )$ . Then $\varphi $ is an algebra homomorphism $\mathrm {alg}({\mathscr C\,}^\sharp _{F^\sharp })\rightarrow {\mathbb P}_V$ satisfying

  1. (i) $\sum _{A\in {\mathscr C\,}^\sharp }\mathrm {m}(\pi _g\varphi (A)\Delta \varphi (gA))\le \delta ^\sharp $ for all $g\in F^\sharp $ , and

  2. (ii) $\sum _{A\in {\mathscr C\,}^\sharp _{F^\sharp }}|\mathrm {m}(\varphi (A))-\mu (A)|\le \delta ^\sharp .$

Let $g\in T$ and $A\in {\mathscr C}_g$ . Then we have $l, g_1, \ldots , g_l, k_1, \ldots , k_l$ as above. Denote by $W_{g, A}''$ the set $\bigcup _{1\le j\le l}(\pi _{g_jg_{j-1}\cdots g_1}^{-1}(\varphi (g_jg_{j-1}\cdots g_1A))\Delta \varphi (A))$ . Then

$$ \begin{align*} \mathrm{m}(W_{g, A}'')&\le \sum_{j=1}^l\mathrm{m}(\pi_{g_jg_{j-1}\cdots g_1}^{-1}(\varphi(g_jg_{j-1}\cdots g_1A))\Delta \varphi(A))\\ &=\sum_{j=1}^l\mathrm{m}(\varphi(g_jg_{j-1}\cdots g_1A)\Delta \pi_{g_jg_{j-1}\cdots g_1}\varphi(A))\le C\delta^\sharp. \end{align*} $$

Also set $W_g''=\bigcup _{A\in {\mathscr C}_g}W_{g, A}''$ and $W''=\bigcup _{g\in T}W_g''$ . Then

$$ \begin{align*} \mathrm{m}(W_g'')\le |{\mathscr C}_g|C\delta^\sharp\le C^2n^C\Big(\max_{1\le k\le n}|S_k|\Big)^C\delta^\sharp \end{align*} $$

and

$$ \begin{align*} \mathrm{m}(W'')\le |T|C^2n^C\Big(\max_{1\le k\le n}|S_k|\Big)^C\delta^\sharp=D\delta^\sharp. \end{align*} $$

Set $W'=\bigcup _{g\in T}(\pi _g^{-1}(\varphi (W)\cap V_{F^\sharp })\setminus \varphi (g^{-1}W))$ . Note that

$$ \begin{align*} W'=\bigcup_{g\in T}(\pi_{g^{-1}}(\varphi(W)\cap V_{F^\sharp})\setminus \varphi(g^{-1}W))\subseteq \bigcup_{g\in T}(\pi_{g^{-1}}\varphi(W)\setminus \varphi(g^{-1}W)), \end{align*} $$

and hence

$$ \begin{align*} \mathrm{m}(W')\le \sum_{g\in T}\mathrm{m}(\pi_{g^{-1}}\varphi(W)\Delta \varphi(g^{-1}W))\le |T|\delta^\sharp. \end{align*} $$

Set $W^*=(\varphi (W)\cap V_{F^\sharp })\setminus (W'\cup W'')$ , and $W^\dagger =W^*\cup \pi _{e_G}^{-1}(V\setminus \bigcup _{g\in S}\pi _gW^*)$ . Then $\bigcup _{g\in S}\pi _gW^\dagger =V$ , verifying condition (ii) in Definition 3.1.

We have

$$ \begin{align*} \mathrm{m}\bigg(\bigcup_{g\in S}\pi_gW^*\bigg)&\ge \mathrm{m}\bigg(\bigcup_{g\in S}\pi_g\varphi(W)\bigg)-|S|\mathrm{m}(W'\cup W''\cup(V\setminus V_{F^\sharp}))\\ &\ge \mathrm{m}\bigg(\varphi\bigg(\bigcup_{g\in S}gW\bigg)\bigg)-\mathrm{m}\bigg(\bigg(\bigcup_{g\in S}\pi_g\varphi(W)\bigg)\Delta \varphi\bigg(\bigcup_{g\in S}gW\bigg)\bigg) \\ & \qquad\qquad\qquad\quad\quad \ -|S|(|T|\delta^\sharp+D\delta^\sharp+\delta^\sharp)\\ &= 1-\mathrm{m}\bigg(\bigg(\bigcup_{g\in S}\pi_g\varphi(W)\bigg)\Delta \bigcup_{g\in S}\varphi(gW)\bigg)-|S|(|T|+D+1)\delta^\sharp\\ &\ge 1-\sum_{g\in S}\mathrm{m}(\pi_g\varphi(W)\Delta \varphi(gW))-|S|(|T|+D+1)\delta^\sharp\\ &\ge 1-|S|\delta^\sharp-|S|(|T|+D+1)\delta^\sharp\ge 1-\delta, \end{align*} $$

and hence

$$ \begin{align*} \mathrm{m}(W^\dagger\setminus W^*)\le \mathrm{m}\bigg(V\setminus \bigcup_{g\in S}\pi_gW^*\bigg)\le \delta. \end{align*} $$

Put ${\mathcal V}_k^\dagger =\varphi ({\mathcal V}_k)$ for $1\le k\le n$ , $S_{n+1}=T\in \overline {{\mathcal F}}(G)$ , and

$$ \begin{align*} {\mathcal V}_{n+1}^\dagger=\bigcup_{g\in T}((W^\dagger\setminus W^*)\cup \pi_g(W^\dagger\setminus W^*)\cup \pi_g^{-1}(W^\dagger\setminus W^*)). \end{align*} $$

Then

$$ \begin{align*} \mathrm{m}({\mathcal V}_{n+1}^\dagger)\le (2|T|+1)\mathrm{m}(W^\dagger\setminus W^*)\le 3\delta |T|, \end{align*} $$

and hence

$$ \begin{align*} \sum_{k=1}^{n+1}\kern-1.5pt\Upsilon(S_k)\mathrm{m}({\mathcal V}_k^\dagger)\le 3\delta |T|\Upsilon(T)+\kern-1pt\sum_{k=1}^n\kern-1.5pt\Upsilon(S_k)(\mu({\mathcal V}_k)+\delta^\sharp)\le \frac14 + \frac12 +\delta^\sharp\kern-1pt\sum_{k=1}^n\kern-1.5pt\Upsilon(S_k)\le 1, \end{align*} $$

verifying condition (i) in Definition 3.1.

Let $g\in T$ and $w_1, w_2\in W^\dagger $ with $\pi _gw_1=w_2$ . If $w_1\not \in W^*$ or $w_2\not \in W^*$ , then $(w_1, w_2)$ is an $S_{n+1}$ -edge with both endpoints in ${\mathcal V}_{n+1}^\dagger $ . Thus we may assume that $w_1, w_2\in W^*$ . Then $w_1=\pi _g^{-1}w_2\in \pi _g^{-1}(\varphi (W)\cap V_{F^\sharp })$ . Since $w_1\notin W'$ , we get $w_1\in \varphi (g^{-1}W)$ . Thus

$$ \begin{align*} w_1\in \varphi(W)\cap \varphi(g^{-1}W)=\varphi(W\cap g^{-1}W)=\varphi\bigg(\bigcup_{A\in {\mathscr C}_g}A\bigg)=\bigcup_{A\in {\mathscr C}_g}\varphi(A). \end{align*} $$

We have $w_1\in \varphi (A)$ for some $A\in {\mathscr C}_g$ . Let $l, g_1, \ldots , g_l, k_1, \ldots , k_l$ be as above for this A. Then for all $1\le j\le l$ the sets $g_{j-1}\cdots g_1A$ and $g_jg_{j-1}\cdots g_1A$ are contained in ${\mathcal V}_{k_j}$ . Since $w_1\notin W_{g, A}''$ , we have $\pi _{g_jg_{j-1}\cdots g_1}w_1\in \varphi (g_jg_{j-1}\cdots g_1A)$ for all $1\le j\le l$ . Thus $\pi _{g_{j-1}\cdots g_1}w_1, \pi _{g_jg_{j-1}\cdots g_1}w_1\in \varphi ({\mathcal V}_{k_j})={\mathcal V}_{k_j}^\dagger $ for all $1\le j\le l$ . Therefore $w_1$ and $w_2$ are connected by a path of length l in which each edge is an $S_k$ -edge with both endpoints in ${\mathcal V}_k^\dagger $ for some $1\le k\le n$ , verifying condition (iii) in Definition 3.1.

Theorem 3.11. Consider the following conditions for an infinite G:

  1. (i) G has property SC;

  2. (ii) every free p.m.p. action $G\curvearrowright (X, \mu )$ has property SC;

  3. (iii) there exists a non-trivial Bernoulli action of G with property SC;

  4. (iv) there exists a non-trivial Bernoulli action of G with property sofic SC;

  5. (v) G has property sofic SC;

  6. (vi) G is neither locally finite nor finitely generated and virtually free.

We have (i) $\Leftrightarrow $ (ii) $\Leftrightarrow $ (iii) $\Rightarrow $ (iv) $\Leftrightarrow $ (v) $\Rightarrow $ (vi). Moreover, when G is amenable all of these conditions are equivalent.

Proof. The equivalence of (i)–(iii) is the content of [Reference Kerr and Li25, Proposition 3.5]. For (iii) $\Rightarrow $ (iv) apply Proposition 3.10. The implication (iv) $\Rightarrow $ (v) follows from the fact that non-trivial Bernoulli actions have positive sofic entropy with respect to every sofic approximation sequence [Reference Bowen5, Reference Kerr21, Reference Kerr and Li22], while (v) $\Rightarrow $ (iv) follows from the definitions and (v) $\Rightarrow $ (vi) from Propositions 3.6 and 3.7.

In the case that G is amenable, [Reference Kerr and Li25, Proposition 3.28] asserts that (vi) $\Leftrightarrow $ (i), which gives us the equivalence of all of the conditions.

A subgroup $G_0$ of G is said to be w-normal in G if there are a countable ordinal $\gamma $ and a subgroup $G_\lambda $ of G for each ordinal $0\le \lambda \le \gamma $ such that:

  1. (i) for any $\lambda <\lambda '\le \gamma $ one has $G_\lambda \subseteq G_{\lambda '}$ ;

  2. (ii) $G=G_\gamma $ ;

  3. (iii) for each $\lambda <\gamma $ the group $G_\lambda $ is normal in $G_{\lambda +1}$ ;

  4. (iv) for each limit ordinal $\lambda '\le \gamma $ one has $G_{\lambda '}=\bigcup _{\lambda <\lambda '}G_\lambda $ .

In conjunction with Theorem 3.11 above, [Reference Kerr and Li25, Theorem 3.29] yields the following result.

Theorem 3.12. Suppose that G has a w-normal subgroup $G_0$ which is amenable but neither locally finite nor virtually cyclic. Then G has property sofic SC.

3.4 W-normal subgroups and property sofic SC

The proof of the following lemma applies some of the ideas from [Reference Austin3, §8.1] to the sofic framework.

Lemma 3.13. Suppose that G is finitely generated and not virtually cyclic, and let A be a generating set for G in $\overline {{\mathcal F}}(G)$ . Then there is a constant $b>0$ such that given any

  1. (i) group H containing G as a subgroup,

  2. (ii) finite subset F of H, and

  3. (iii) $r, M\in {\mathbb N}$ and $\delta>0$

one can find, for any good enough sofic approximation $\pi : H\rightarrow \operatorname {\mathrm {Sym}}(V)$ for H, sets $Z\subseteq {\mathcal V}\subseteq V_F$ , where $V_F$ denotes the set of all $v\in V$ satisfying $\pi _{gh}=\pi _g\pi _hv$ for all $g, h\in F$ and $\pi _gv\neq \pi _hv$ for all distinct $g, h\in F$ , such that $|\bigcup _{g\in A^{2r}}\pi _g{\mathcal V}|/|V|\ge 1-\delta $ , $|{\mathcal V}|\le b|V|/r$ , $|Z|\le |V|/M$ , and every point of ${\mathcal V}$ is connected to some point of Z by an A-path of length at most $2M$ with all vertices in ${\mathcal V}$ .

Proof. Since G is not virtually cyclic, there exists a $c>0$ such that $|A^n| \geq cn^2$ for all $n\in {\mathbb N}$ [Reference Mann29, Corollary 3.5]. Set $b=5/c$ . Let $H, F, r, M, \delta $ , and $\pi $ be as in the lemma statement. Set $N=|A|^{3M}$ . Take $k\in {\mathbb N}$ such that $|A^{kr}|\ge N|A^{2r}|$ .

Denote by $V'$ the set of all $v\in V$ satisfying $\pi _{gh}v=\pi _g\pi _hv$ for all $g, h\in (F\cup A)^{100(M+r)}$ and $\pi _gv\neq \pi _hv$ for all distinct $g, h\in (F\cup A)^{100(M+r)}$ . Denote by $V''$ the set of all $v\in V$ satisfying $\pi _{gh}v=\pi _g\pi _hv$ for all $g, h\in (F\cup A)^{(200+k)(M+r)}$ and $\pi _gv\neq \pi _hv$ for all distinct $g, h\in (F\cup A)^{(200+k)(M+r)}$ . Then $\pi _gV''\subseteq V'$ for every $g\in A^{(k+6)r}$ . Assuming that $\pi $ is a good enough sofic approximation, we have $|V''|/|V|\ge 1-\delta $ . Take a maximal $(A,r)$ -separated subset W of $V''$ , and also take a maximal $(A, r)$ -separated subset $W'$ of $V'$ containing W. Then we have $\bigcup _{g\in A^{2r}}\pi _gW\supseteq V''$ , and hence

$$ \begin{align*} \frac{1}{|V|} \bigg|\bigcup_{g\in A^{2r}}\pi_gW\bigg| \ge \frac{|V''|}{|V|} \ge 1-\delta. \end{align*} $$

Let $w\in W$ . Set $T_w=W'\cap \pi _{A^{(k+2)r}}w$ . Note that $\pi _{A^{kr}}w\subseteq V'\subseteq \pi _{A^{2r}}W'$ . For each $g\in A^{kr}$ we have $\pi _gw\in \pi _{A^{2r}}z$ for some $z\in W'$ . Then $z\in \pi _{A^{2r}}\pi _gw\subseteq \pi _{A^{(k+2)r}}w$ , and hence $z\in T_w$ . Thus

$$ \begin{align*} \pi_{A^{kr}}w\subseteq \pi_{A^{2r}}T_w. \end{align*} $$

Therefore

$$ \begin{align*} |T_w|\ge \frac{|A^{kr}|}{|A^{2r}|}\ge N. \end{align*} $$

Set $T=\bigcup _{w\in W}T_w\subseteq W'$ . We have

$$ \begin{align*} |A^r| |W'| = \bigg| \bigsqcup_{w\in W'} \pi_{A^r} w \bigg| \leq |V| \end{align*} $$

whence

(3) $$ \begin{align} |T|\le |W'| \leq \frac{|V|}{|A^r|} \leq \frac{|V|}{cr^2}. \end{align} $$

Let $w\in W$ . Let $(T_w, E_w)$ be the graph whose edges are those pairs of vertices which can be joined by an A-path of length at most $4r+1$ , and let us show that it is connected. It is enough to demonstrate that a given $v\in T_w$ is connected to w by a path in $(T_w, E_w)$ . Choose a shortest A-path from w to v. For each vertex z in this path contained in $\pi _{A^{kr}}w$ , the fact that $z\in \pi _{A^{kr}}w\subseteq \pi _{A^{2r}}T_w$ means that we can connect z to some $u_z\in T_w$ by an A-path $p_z$ of length at most $2r$ . By inserting $p_z$ and its reverse at z, we construct an A-path from w to v in which points of $T_w$ appear in every interval of length $4r+1$ . Therefore v is connected to w by some path in $(T_w, E_w)$ , showing that $(T_w, E_w)$ is connected.

Consider the graph $(T , E )$ whose edges are those pairs of vertices which can be joined by an A-path of length at most $4r+1$ . From the above, every connected component of this graph has at least N points. Starting with $(T , E )$ , we recursively build a sequence of graphs with vertex set T by removing one edge at each stage so as to destroy some cycle at that stage, until there are no more cycles left and we arrive at a subgraph $(T, E')$ such that $(T, E)$ and $(T, E')$ have the same connected components and each connected component of $(T, E')$ is a tree.

For each pair $(v,w)$ in $E'$ , we choose an A-path in $\pi _{A^{4r}}T$ joining v to w of length at most $4r+1$ . Denote by ${\mathcal V}$ the collection of all vertices which appear in one of these paths. Then ${\mathcal V}\subseteq \pi _{A^{4r}}T\subseteq V'\subseteq V_F$ . Note that each A-connected component of ${\mathcal V}$ has at least N points, and $W\subseteq T\subseteq {\mathcal V}$ . Thus

$$ \begin{align*} \frac{1}{|V|} \bigg|\bigcup_{g\in A^{2r}}\pi_g{\mathcal V}\bigg| \ge \frac{1}{|V|} \bigg|\bigcup_{g\in A^{2r}}\pi_gW\bigg| \ge 1-\delta. \end{align*} $$

Moreover, using (3) we have

$$ \begin{align*} |{\mathcal V}| \leq |T|+4r|E'| \leq (4r+1)|T| \leq 5r\cdot \frac{|V|}{cr^2} =\frac{b|V|}{r}. \end{align*} $$

Let ${\mathcal C}$ be an A-connected component of ${\mathcal V}$ . Denote by $({\mathcal C}, E_{{\mathcal C}})$ the graph whose edges are the pairs $(w, v)\in {\mathcal C}^2$ such that $\pi _gw=v$ for some $g\in A$ . Then $({\mathcal C}, E_{{\mathcal C}})$ is connected. Endow ${\mathcal C}$ with the geodesic distance $\rho $ induced from $E_{{\mathcal C}}$ . Take a maximal subset $Z_{{\mathcal C}}$ of ${\mathcal C}$ which is $(\rho , M)$ -separated in the sense that the M-balls $\{ v\in {\mathcal C} : \rho (v,z) \leq M \}$ for $z\in Z_{{\mathcal C}}$ are pairwise disjoint. Then $Z_{{\mathcal C}}$ is $(\rho , 2M)$ -spanning in ${\mathcal C}$ , that is, every point of ${\mathcal C}$ is connected to some point of $Z_{\mathcal C}$ by an A-path of length at most $2M$ with all vertices in ${\mathcal C}$ . Since $|{\mathcal C}|\ge N=|A|^{3M}>|A|^{2M}$ , we have $|Z_{{\mathcal C}}|\ge 2$ . Then $|{\mathcal C}\cap \pi _{A^{M}}z|\ge M$ for every $z\in Z_{{\mathcal C}}$ . Since the sets ${\mathcal C}\cap \pi _{A^M}z$ for $z\in Z_{{\mathcal C}}$ are pairwise disjoint, we get

$$ \begin{align*} |Z_{{\mathcal C}}|M\le \sum_{z\in Z_{{\mathcal C}}}|{\mathcal C}\cap \pi_{A^M}z|\le |{\mathcal C}|. \end{align*} $$

Denote by Z the union of the sets $Z_{{\mathcal C}}$ where ${\mathcal C}$ runs over all A-connected components of ${\mathcal V}$ . Then every point of ${\mathcal V}$ is connected to some point of Z by an A-path of length at most $2M$ with all vertices in ${\mathcal V}$ , and $|Z|/|V|\le 1/M$ .

For the definition of w-normality, see the paragraph before Theorem 3.12.

Proposition 3.14. Suppose that G has a w-normal subgroup $G^\flat $ with property sofic SC. Then G has property sofic SC.

Proof. Suppose first that $G^\flat $ is locally virtually cyclic. Then $G^\flat $ is amenable and, by Lemma 3.5 and Theorem 3.11, neither locally finite nor virtually cyclic. It follows by Theorem 3.12 that G has property sofic SC, as desired.

Suppose now that $G^\flat $ is not locally virtually cyclic. In this case we will first set out the argument under the assumption that $G^\flat $ is normal in G. Take a finitely generated subgroup $G_0$ of $G^\flat $ such that $G_0$ is not virtually cyclic. Take an $S_1\in \overline {{\mathcal F}}(G_0)$ generating $G_0$ . Let $b> 0$ be as given by Lemma 3.13 for the group $G_0$ and generating set $S_1$ .

Let $\Upsilon $ be a function ${\mathcal F}(G)\rightarrow [0, \infty )$ . Choose an $r\in {\mathbb N}$ large enough so that

(4) $$ \begin{align} 3b\Upsilon(S_1)\leq r. \end{align} $$

Set $S=S_1^{2r}\in \overline {{\mathcal F}}(G_0)$ .

Consider the restriction of $3\Upsilon $ to ${\mathcal F}(G^\flat )$ . Since $G^\flat $ has property sofic SC, there exists an $S^\flat \in \overline {{\mathcal F}}(G^\flat )$ such that for any $T^\flat \in \overline {{\mathcal F}}(G^\flat )$ there are $C^\flat , n^\flat \in {\mathbb N}$ and $S^\flat _1, \ldots , S^\flat _{n^\flat }\in \overline {{\mathcal F}}(G^\flat )$ such that for any good enough sofic approximation $\pi : G\rightarrow \operatorname {\mathrm {Sym}}(V)$ for G there are subsets $W^\flat $ and ${\mathcal V}^\flat _k$ of V for $1\le k\le n^\flat $ satisfying the following conditions:

  1. (i) $\sum _{k=1}^{n^\flat } 3\Upsilon (S^\flat _{k})\mathrm {m}({\mathcal V}^\flat _{k})\le 1$ ;

  2. (ii) $\bigcup _{g\in S^\flat }\pi _gW^\flat =V$ ;

  3. (iii) if $w_1, w_2\in W^\flat $ satisfy $\pi _gw_1=w_2$ for some $g\in T^\flat $ then $w_1$ and $w_2$ are connected by a path of length at most $C^\flat $ in which each edge is an $S^\flat _k$ -edge with both endpoints in ${\mathcal V}^\flat _k$ for some $1\le k\le n^\flat $ .

Let $T\in \overline {{\mathcal F}}(G)$ . Set

$$ \begin{align*} S_2=S^\flat T S^\flat \in \overline{{\mathcal F}}(G). \end{align*} $$

Take an $M\in {\mathbb N}$ large enough so that

(5) $$ \begin{align} M\ge 12\Upsilon(S_2)|S_2|. \end{align} $$

Set $T^\flat =\bigcup _{g\in T}(S^\flat S_1^{2M}gS_1^{2M}g^{-1}S^\flat \cup S^\flat gS_1^{2M}g^{-1}S_1^{2M}S^\flat )\in \overline {{\mathcal F}}(G^\flat )$ . Then we have $C^\flat $ , $n^\flat $ , and $S^\flat _{k}$ for $1\le k\le n^\flat $ as above. Set

$$ \begin{align*} C=4M+2+C^\flat\in {\mathbb N}, \end{align*} $$

and $F=(S_1\cup T\cup S^\flat \cup \bigcup _{k=1}^{n^\flat }S_k^\flat )^{100MCr}\in {\mathcal F}(G)$ .

Now let $\pi : G\rightarrow \operatorname {\mathrm {Sym}}(V)$ be a good enough sofic approximation for G. By Lemma 3.13 we can find sets $Z\subseteq {\mathcal V}_1\subseteq V_F$ , where $V_F$ denotes the set of $v\in V$ satisfying $\pi _{gh}=\pi _g\pi _hv$ for all $g, h\in F$ and $\pi _gv\neq \pi _hv$ for all distinct $g, h\in F$ , such that $\mathrm {m}(\bigcup _{g\in S}\pi _g{\mathcal V}_1)\ge 1-1/M$ , $\mathrm {m}({\mathcal V}_1)\le b/r$ , $\mathrm {m}(Z)\le 1/M$ , and every point of ${\mathcal V}_1$ is connected to some point of Z by an $S_1$ -path of length at most $2M$ with all vertices in ${\mathcal V}_1$ . Note that

Set $W={\mathcal V}_1\cup \pi _{e_G}^{-1}(V\setminus \bigcup _{g\in S}\pi _g {\mathcal V}_1)\subseteq V$ . Then $\bigcup _{g\in S}\pi _g W=V$ , which verifies condition (ii) in Definition 3.1.

Set ${\mathcal V}_2=(\bigcup _{g\in T}((W\setminus {\mathcal V}_1)\cup \pi _g (W\setminus {\mathcal V}_1)\cup \pi _g^{-1}(W\setminus {\mathcal V}_1)))\cup \bigcup _{g\in S_2}\pi _g Z\subseteq V$ . Then

$$ \begin{align*} \mathrm{m}({\mathcal V}_2)\le 3|T|\mathrm{m}(W\setminus {\mathcal V}_1)+|S_2|\mathrm{m}(Z)\le 3|S_2|\mathrm{m}\bigg(\!V\setminus \bigcup_{g\in S}\pi_g {\mathcal V}_1\!\bigg)+|S_2|/M\le 4|S_2|/M, \end{align*} $$

and hence

Assuming that $\pi $ is a good enough sofic approximation for G, we have $W^\flat $ and ${\mathcal V}^\flat _{k}$ for $1\le k\le n^\flat $ as above, in which case

$$ \begin{align*} \sum_{k=1}^{n^\flat}\Upsilon(S^\flat_{k})\mathrm{m}({\mathcal V}^\flat_{k})\le \frac{1}{3}. \end{align*} $$

Putting the above estimates together, we get

$$ \begin{align*} \Upsilon(S_1)\mathrm{m}({\mathcal V}_1)+\Upsilon(S_2)\mathrm{m}({\mathcal V}_2)+\sum_{k=1}^{n^\flat}\Upsilon(S^\flat_{k})\mathrm{m}({\mathcal V}^\flat_{k})\le 1, \end{align*} $$

which verifies condition (i) in Definition 3.1.

Let $g\in T$ and $w_1, w_2\in W$ be such that $\pi _gw_1=w_2$ . If either $w_1\in W\setminus {\mathcal V}_1$ or $w_2\in W\setminus {\mathcal V}_1$ , then $(w_1, w_2)$ is an $S_2$ -edge with both endpoints in ${\mathcal V}_2$ . Thus we may assume that $w_1, w_2\in {\mathcal V}_1$ . For $i=1, 2$ , we can connect $w_i$ to some $z_i\in Z$ by an $S_1$ -path of length at most $2M$ with all vertices in ${\mathcal V}_1$ . Then $w_i=\pi _{t_i}z_i$ for some $t_i\in S_1^{2M}$ . We have $\pi _gz_1=\pi _{a_1} u_1$ for some $u_1\in W^\flat $ and $a_1\in S^\flat $ , and $z_2= \pi _{a_2} u_2$ for some $u_2\in W^\flat $ and $a_2\in S^\flat $ . Note that $a_1^{-1}g$ and $a_2^{-1}$ are both in $S_2$ . Since $\pi _{a_1^{-1}g}z_1=u_1$ , the pair $(z_1, u_1)$ is an $S_2$ -edge with both endpoints in ${\mathcal V}_2$ . Also, since $\pi _{a_2^{-1}}z_2=u_2$ the pair $(w_2, u_2)$ is an $S_2$ -edge with both endpoints in ${\mathcal V}_2$ . Note that

$$ \begin{align*} \pi_{a_2^{-1}t_2^{-1}gt_1g^{-1}a_1} u_1&=\pi_{a_2^{-1}}\pi_{t_2^{-1}}\pi_{g}\pi_{t_1}\pi_{g^{-1}}\pi_{a_1} u_1\\ &=\pi_{a_2^{-1}}\pi_{t_2^{-1}}\pi_g\pi_{t_1}z_1\\ &=\pi_{a_2^{-1}}\pi_{t_2^{-1}}\pi_g w_1\\ &=\pi_{a_2^{-1}}\pi_{t_2^{-1}}w_2\\ &=\pi_{a_2^{-1}}z_2\\ &=u_2. \end{align*} $$

Since $a_2^{-1}t_2^{-1}gt_1g^{-1}a_1\in S^\flat S_1^{2M}gS_1^{2M}g^{-1}S^\flat \subseteq T^\flat $ , this means that $u_2\in \pi _{T^\flat }u_1$ . Then $u_1$ and $u_2$ are connected by a path of length at most $C^\flat $ in which each edge is an $S^\flat _k$ -edge with both endpoints in ${\mathcal V}^\flat _k$ for some $1\le k\le n^\flat $ . Therefore $w_1$ and $w_2$ are connected by a path of length at most $4M+2+C^\flat =C$ in which each edge is either an $S_j$ -edge with both endpoints in ${\mathcal V}_j$ for some $1\le j\le 2$ or an $S^\flat _k$ -edge with both endpoints in ${\mathcal V}^\flat _k$ for some $1\le k\le n^\flat $ , verifying condition (iii) in Definition 3.1.

Notice that the set S used in the above verification of property sofic SC for G is contained in $G_0$ , which can be any non-virtually-cyclic finitely generated subgroup of $G^\flat $ , and only depends on the restriction of $\Upsilon $ to $\overline {{\mathcal F}}(G_0)$ . This has the consequence that if $G_1 , G_2 , \ldots $ is a sequence of countable groups such that $G_n$ is a normal subgroup of $G_{n+1}$ for each n and $G_1$ is not locally virtually cyclic and has property sofic SC then the group $\bigcup _{n=1}^\infty G_n$ has property sofic SC. Indeed, we can fix a finitely generated subgroup $G_1'$ of $G_1$ which is not virtually cyclic and apply the above argument recursively, taking $G_0 = G_1'$ , $G^\flat = G_n$ , and $G=G_{n+1}$ at the nth stage to deduce that $G_{n+1}$ has property sofic SC, and if the function $\Upsilon $ is taken at each stage to be the restriction of a prescribed function ${\mathcal F} (\bigcup _{n=1}^\infty G_n ) \to [0,\infty )$ then we can use the same set S for all n, showing that $\bigcup _{n=1}^\infty G_n$ has property sofic SC. It follows by ordinal well-ordering that if $G^\flat $ is merely assumed to be w-normal in G then we can still conclude that G has property sofic SC.

3.5 Product groups

Let G and H be countable groups. Let $\pi : G\to \operatorname {\mathrm {Sym}} (V)$ and $\sigma : H\to \operatorname {\mathrm {Sym}} (W)$ be sofic approximations. The product sofic approximation $\pi \times \sigma : G\times H \to \operatorname {\mathrm {Sym}} (V\times W)$ is defined by

$$ \begin{align*} (\pi\times\sigma )_{(g,h)} (v,w) = (\pi_g (v) , \sigma_h (w)) \end{align*} $$

for all $g\in G$ , $h\in H$ , $v\in V$ , and $w\in W$ . Note that if $\{ \pi _k \}$ and $\{ \sigma _k \}$ are sofic approximation sequences for G and H, respectively, then $\{ \pi _k\times \sigma _k \}$ is a sofic approximation sequence for $G\times H$ .

Proposition 3.15. Let G and H be countably infinite groups. Let ${\mathscr S}$ be the collection of product sofic approximations for $G\times H$ . Then $G\times H$ has property ${\mathscr S}$ -SC if and only if at least one of G and H is not locally finite.

Proof. If G and H are both locally finite then $G\times H$ is locally finite and hence does not have property ${\mathscr S}$ -SC by Proposition 3.6. Suppose then that at least one of G and H is not locally finite. Take two non-trivial Bernoulli actions $G\curvearrowright (X,\mu )$ and $H\curvearrowright (Y,\nu )$ . By [Reference Kerr and Li25, Proposition 3.32] the p.m.p. action $G\times H\curvearrowright (X \times Y ,\mu \times \nu )$ given by $(g,h)(x,y) = (gx,hy)$ for all $g\in G$ , $h\in H$ , $x\in X$ , and $y\in Y$ has property SC, and hence has property sofic SC by Proposition 3.10.

By [Reference Bowen5, Reference Kerr21], for every finite partition ${\mathscr C}$ of X, $F\in {\mathcal F} (G)$ containing $e_G$ , and $\delta> 0$ one has $\operatorname {\mathrm {Hom}}_\mu ({\mathscr C} , F,\delta ,\pi ) \neq \emptyset $ for every sufficiently good sofic approximation $\pi $ for G, and for every finite partition ${\mathscr D}$ of Y, $L\in {\mathcal F} (H)$ containing $e_H$ , and $\delta> 0$ one has $\operatorname {\mathrm {Hom}}_\nu ({\mathscr D} , L,\delta ,\sigma ) \neq \emptyset $ for every sufficiently good sofic approximation $\sigma $ for H. Given such sofic approximations $\pi : G\to \operatorname {\mathrm {Sym}} (V)$ and $\sigma : H\to \operatorname {\mathrm {Sym}} (W)$ and $\varphi \in \operatorname {\mathrm {Hom}}_\mu ({\mathscr C} , F,\delta ,\pi )$ and $\psi \in \operatorname {\mathrm {Hom}}_\nu ({\mathscr D} , L,\delta ,\sigma )$ , we have a homomorphism $\zeta : \mathrm {alg} ({\mathscr C}_F \times {\mathscr D}_L ) = \mathrm {alg} (({\mathscr C}\times {\mathscr D} )_{F\times L} )\to {\mathbb P}_{V\times W}$ determined by $\zeta (C\times D) = \varphi (C)\times \psi (D)$ for $C\in {\mathscr C}_F$ and $D\in {\mathscr D}_L$ , and one can readily verify that $\zeta $ belongs to $\operatorname {\mathrm {Hom}}_{\mu \times \nu } ({\mathscr C}\times {\mathscr D} , F\times L,2\delta ,\pi \times \sigma )$ , showing that this set of homomorphisms is non-empty. Since the algebra of subsets of $X\times Y$ generated by products of finite partitions is dense in the $\sigma $ -algebra with respect to the pseudometric $d(A,B) = (\mu \times \nu )(A\Delta B)$ , it follows by a simple approximation argument that for every finite partition ${\mathscr E}$ of $X\times Y$ , finite set $e_{G\times H} \in K\subseteq G\times H$ , and $\delta> 0$ one has $\operatorname {\mathrm {Hom}}_{\mu \times \nu } ({\mathscr E} , K,\delta ,\pi \times \sigma )\neq \emptyset $ for all good enough sofic approximations $\pi : G\to \operatorname {\mathrm {Sym}} (V)$ and $\sigma : H\to \operatorname {\mathrm {Sym}} (W)$ . Since the action $G\times H\curvearrowright (X \times Y ,\mu \times \nu )$ has property sofic SC, it follows that $G\times H$ has property ${\mathscr S}$ -SC.

3.6 Property sofic SC under continuous orbit equivalence

Proposition 3.16. Let $G\curvearrowright X$ and $H\curvearrowright Y$ be topologically free continuous actions on compact metrizable spaces which are continuously orbit equivalent. Suppose that $G\curvearrowright X$ has property sofic SC. Then $H\curvearrowright Y$ has property sofic SC.

To prove this proposition we may assume that $X=Y$ and that the identity map of X provides a continuous orbit equivalence between the actions $G\curvearrowright X$ and $H\curvearrowright X$ . Let $\kappa : G\times X\rightarrow H$ and $\lambda : H\times X \rightarrow G$ be the associated cocycles.

The actions of G and H generate an action $G*H \curvearrowright X$ of their free product via the canonical embeddings of G and H into $G*H$ . Since the actions of G and H are topologically free, we can find a G-invariant dense $G_\delta $ set $W_1 \subseteq X$ on which G acts freely and an H-invariant dense $G_\delta $ set $W_2 \subseteq X$ on which H acts freely. Set $X_0 = \bigcap _{s\in G*H} s(W_1 \cap W_2 )$ . Then $X_0$ is a $G*H$ -invariant dense $G_\delta $ subset of X on which both G and H act freely.

Fix a compatible metric d on X which gives X diameter no bigger than $1$ . For each $g\in G$ there is an $\eta _g>0$ such that for any $x, y\in X$ with $d(x, y)\le \eta _g$ one has $\kappa (g, x)=\kappa (g, y)$ , and likewise for each $s\in H$ there is an $\eta _s>0$ such that for any $x, y\in X$ with $d(x, y)\le \eta _s$ one has $\lambda (s, x)=\lambda (s, y)$ . We put $\eta _F=\min _{g\in F}\eta _g>0$ for a non-empty finite set $F\subseteq G$ , and $\eta _L=\min _{s\in L}\eta _s>0$ for a non-empty finite set $L\subseteq H$ .

We will need the following lemma, which will also be of use in the proof of Theorem 4.1.

Lemma 3.17. Let $L\in \overline {{\mathcal F}}(H)$ , and $0<\tau <1$ . Set $F=\lambda (L^2, X)\in \overline {{\mathcal F}}(G)$ and

$$ \begin{align*} \tau'=\min\{\eta_{L^2}\tau^{1/2}/(8|F|)^{1/2}, \tau/(22|F|^2)\}>0. \end{align*} $$

Let $\pi : G\rightarrow \operatorname {\mathrm {Sym}}(V)$ be an $(F, \tau ')$ -approximation for G. Let $\varphi \in \operatorname {\mathrm {Map}}_d(F, \tau ', \pi )$ be such that $\varphi (V)\subseteq X_0$ . Define $\sigma ': H\rightarrow V^V$ by

$$ \begin{align*} \sigma^{\prime}_tv=\pi_{\lambda(t, \varphi(v))}v \end{align*} $$

for $t\in H$ and $v\in V$ . Then there is an $(L, \tau )$ -approximation $\sigma : H\rightarrow \operatorname {\mathrm {Sym}}(V)$ for H such that $\rho _{\mathrm {Hamm}}(\sigma _t, \sigma ^{\prime }_t)\le \tau $ for all $t\in L^2$ .

Proof. Denote by $V_F$ the set of all $v\in V$ satisfying $\pi _g\pi _hv=\pi _{gh}v$ for all $g, h\in F$ and $\pi _gv\neq \pi _hv$ for all distinct $g, h\in F$ . Then

$$ \begin{align*} \mathrm{m} (V\setminus V_F)\le 2|F|^2\tau'\le \frac{\tau}{11}. \end{align*} $$

Denote by $V_\varphi $ the set of all $v\in V$ satisfying $d(\varphi (\pi _gv), g\varphi (v))\le \eta _{L^2}$ for all $g\in F$ . Then

$$ \begin{align*} \mathrm{m} (V\setminus V_\varphi )\le |F|\bigg(\frac{\tau'}{\eta_{L^2}}\bigg)^2\le \frac{\tau}{8}. \end{align*} $$

For all $s, t\in L^2$ and $v\in V_F\cap V_\varphi $ , since $\lambda (t, \varphi (v))\in F$ we have

$$ \begin{align*} d(\varphi(\pi_{\lambda(t, \varphi(v))}v), \lambda(t, \varphi(v))\varphi(v))\le \eta_{L^2} \end{align*} $$

and hence

$$ \begin{align*} \lambda(s, \varphi(\pi_{\lambda(t, \varphi(v))}v))=\lambda(s, \lambda(t, \varphi(v))\varphi(v))=\lambda(s, t\varphi(v)), \end{align*} $$

which yields

$$ \begin{align*} \sigma^{\prime}_s\sigma^{\prime}_tv=\pi_{\lambda(s, \varphi(\sigma^{\prime}_tv))}\sigma^{\prime}_tv &=\pi_{\lambda(s, \varphi(\pi_{\lambda(t, \varphi(v))}v))}\pi_{\lambda(t, \varphi(v))}v\\ &=\pi_{\lambda(s, t\varphi(v))}\pi_{\lambda(t, \varphi(v))}v\\ &=\pi_{\lambda(s, t\varphi(v))\lambda(t, \varphi(v))}v\\ &=\pi_{\lambda(st, \varphi(v))}v\\ &=\sigma^{\prime}_{st}v , \end{align*} $$

so that

(6) $$ \begin{align} \rho_{\mathrm{Hamm}}(\sigma^{\prime}_s\sigma^{\prime}_t, \sigma^{\prime}_{st})\le \mathrm{m} (V\setminus (V_F\cap V_\varphi))\le \frac{\tau}{11}+\frac{\tau}{8}=\frac{19\tau}{88}. \end{align} $$

Note that $\sigma ^{\prime }_{e_H}=\pi _{e_G}$ . For each $t\in H$ choose a $\sigma _t\in \operatorname {\mathrm {Sym}}(V)$ such that $\sigma _tv=\sigma ^{\prime }_tv$ for all $v\in V$ satisfying $\sigma ^{\prime }_{t^{-1}}\sigma ^{\prime }_tv=v$ . For each $t\in L^2$ , taking $s=t^{-1}$ in (6) we conclude that

$$ \begin{align*} \rho_{\mathrm{Hamm}}(\sigma_t, \sigma^{\prime}_t)&\le \rho_{\mathrm{Hamm}}(\sigma^{\prime}_{t^{-1}}\sigma^{\prime}_t, \mathrm{id})\\ &\le \rho_{\mathrm{Hamm}}(\sigma^{\prime}_{t^{-1}}\sigma^{\prime}_t, \sigma^{\prime}_{e_H})+\rho_{\mathrm{Hamm}}(\sigma^{\prime}_{e_H}, \mathrm{id})\\ &\le \frac{19\tau}{88}+\rho_{\mathrm{Hamm}}(\pi_{e_G}, \mathrm{id})\\ &\le \frac{19\tau}{88}+\tau'\\ &\le \frac{19\tau}{88}+\frac{\tau}{22}=\frac{23\tau}{88}, \end{align*} $$

which in particular shows that $\rho _{\mathrm {Hamm}}(\sigma _t, \sigma ^{\prime }_t)<\tau $ . For all $s,t \in L$ we then have

$$ \begin{align*} \rho_{\mathrm{Hamm}}(\sigma_s\sigma_t, \sigma_{st})&\le \rho_{\mathrm{Hamm}}(\sigma_s, \sigma^{\prime}_s)+\rho_{\mathrm{Hamm}}(\sigma_t, \sigma^{\prime}_t)+\rho_{\mathrm{Hamm}}(\sigma^{\prime}_s\sigma^{\prime}_t, \sigma^{\prime}_{st})\\&\quad+\rho_{\mathrm{Hamm}}(\sigma_{st}, \sigma^{\prime}_{st})\\ &\le \frac{23\tau}{88} + \frac{23\tau}{88}+\frac{19\tau}{88}+\frac{23\tau}{88}=\tau. \end{align*} $$

For all distinct $s,t\in L^2$ , since $\varphi (V)\subseteq X_0$ we have $\sigma ^{\prime }_sv\neq \sigma ^{\prime }_tv$ for all $v\in V_F$ and hence

$$ \begin{align*} \rho_{\mathrm{Hamm}}(\sigma_s, \sigma_t)&\ge \rho_{\mathrm{Hamm}}(\sigma^{\prime}_s, \sigma^{\prime}_t)-\rho_{\mathrm{Hamm}}(\sigma_s, \sigma^{\prime}_s)-\rho_{\mathrm{Hamm}}(\sigma_t, \sigma^{\prime}_t)\\ &\ge \mathrm{m} (V_F)-\frac{23\tau}{88}-\frac{23\tau}{88}\\ &\ge 1-\frac{\tau}{11}-\frac{23\tau}{44}> 1-\tau. \\ \end{align*} $$

Proof Proof of Proposition 3.16

Let $\Upsilon _H$ be a function ${\mathcal F}(H)\rightarrow [0, \infty )$ . Define the function $\Upsilon _G: {\mathcal F}(G)\rightarrow [0, \infty )$ by $\Upsilon _G(F)=2\Upsilon _H(\kappa (F, X))$ .

Since the action $G\curvearrowright X$ has property sofic SC, there exists an $S_G\in \overline {{\mathcal F}}(G)$ such that for any $T_G\in \overline {{\mathcal F}}(G)$ there are $C_G, n_G\in {\mathbb N}$ , $S_{G, 1}, \ldots , S_{G, n_G}\in \overline {{\mathcal F}}(G)$ , $L_G\in \overline {{\mathcal F}}(G)$ , and $0<\tau _G<1$ such that, for any $(L_G, \tau _G)$ -approximation $\pi : G\rightarrow \operatorname {\mathrm {Sym}}(V)$ for G with $\operatorname {\mathrm {Map}}_d(L_G, \tau _G, \pi )\neq \emptyset $ , there are subsets $W_G$ and ${\mathcal V}_{G, j}$ of V for $1\le j\le n_G$ satisfying the following conditions:

  1. (i) $\sum _{j=1}^{n_G} \Upsilon _G(S_{G, j})\mathrm {m}({\mathcal V}_{G, j})\le 1$ ;

  2. (ii) $\bigcup _{g\in S_G}\pi _gW_G=V$ ;

  3. (iii) if $w_1, w_2\in W_G$ satisfy $\pi _gw_1=w_2$ for some $g\in T_G$ then $w_1$ and $w_2$ are connected by a path of length at most $C_G$ in which each edge is an $S_{G, j}$ -edge with both endpoints in ${\mathcal V}_{G, j}$ for some $1\le j\le n_G$ .

Set $S_H=\kappa (S_G, X)\in \overline {{\mathcal F}}(H)$ .

Let $T_H\in \overline {{\mathcal F}}(H)$ . Set $T_G=\lambda (T_H, X)\in \overline {{\mathcal F}}(G)$ . Then we have $C_G$ , $n_G$ , $S_{G, j}$ for $1\le j\le n_G$ , $L_G$ , and $\tau _G$ as above. Set $C_H=C_G$ , $n_H=n_G+1$ , $S_{H, j}=\kappa (S_{G, j}, X)\in \overline {{\mathcal F}}(H)$ for $1\le j\le n_G$ , and $S_{H, n_H}=T_H\in \overline {{\mathcal F}}(H)$ . Take $0<\delta _H<1/(6\Upsilon _H(T_H)|T_H|)$ . Also, set $A=L_G\cup S_G\cup T_G\cup \bigcup _{j=1}^{n_G}S_{G, j}\in {\mathcal F}(G)$ , $L_H=\kappa (A^{2(100+C_G)}, X)\in {\mathcal F}(H)$ , and

$$ \begin{align*} \tilde{\tau}_G &= \min\{(\tau_G/2)^2, \delta_H/(4|S_G|\cdot|A|^{2(100+C_G)})\}>0, \\ \tau_H &= \min\{\eta_{A^{2(100+C_G)}}\tilde{\tau}_G^{1/2}/(8|L_H|)^{1/2}, \tilde{\tau}_G/(22|L_H|^2), \tau_G/(2|L_H|^{1/2})\}>0. \end{align*} $$

Let $\sigma\kern-1.5pt :\! H\kern-1pt\rightarrow\kern-1pt \operatorname {\mathrm {Sym}}(\kern-0.5pt V\kern-0.5pt)$ be an $(\kern-0.8 ptL_H,\kern-1pt \tau _H\kern-0.8pt)$ -approximation for H with $\operatorname {\mathrm {Map}}_d(\kern-0.8pt L_H,\kern-1pt \tau _H/2,\kern-1pt \sigma \kern-0.8pt)\kern-1.5pt \neq\kern-1.5pt \emptyset $ . Choose a $\varphi \in \operatorname {\mathrm {Map}}_d(L_H, \tau _H/2, \sigma )$ . Since $X_0$ is dense in X, by perturbing $\varphi $ if necessary we may assume that $\varphi \in \operatorname {\mathrm {Map}}_d(L_H, \tau _H, \sigma )$ and $\varphi (V)\subseteq X_0$ . Define $\pi ': G\rightarrow V^V$ by

$$ \begin{align*} \pi^{\prime}_gv=\sigma_{\kappa(g, \varphi(v))}v \end{align*} $$

for all $v\in V$ and $g\in G$ . By Lemma 3.17 there is an $(A^{100+C_G}, \tilde {\tau }_G)$ -approximation $\pi : G\rightarrow \operatorname {\mathrm {Sym}}(V)$ such that $\rho _{\mathrm {Hamm}}(\pi _g, \pi ^{\prime }_g)\le \tilde {\tau }_G$ for all $g\in A^{100+C_G}$ . For each $g\in L_G\subseteq A^{100+C_G}$ we have

$$ \begin{align*} d_2(g\varphi, \varphi\pi_g)&\le d_2(g\varphi, \varphi\pi^{\prime}_g)+d_2(\varphi\pi^{\prime}_g, \varphi\pi_g)\\ &\le \bigg(\frac{1}{|V|}\sum_{v\in V}d(\kappa(g, \varphi(v))\varphi(v), \varphi(\sigma_{\kappa(g, \varphi(v))}v))^2\bigg)^{1/2}+\tilde{\tau}_G^{1/2}\\ &\le \bigg(\frac{1}{|V|}\sum_{v\in V}\sum_{t\in \kappa(g, X)}d(t\varphi(v), \varphi(\sigma_tv))^2\bigg)^{1/2}+\frac{\tau_G}{2}\\ &\le (\tau_H^2|L_H|)^{1/2}+\frac{\tau_G}{2} \\ &\le \tau_G. \end{align*} $$

Thus $\varphi \in \operatorname {\mathrm {Map}}_d(L_G, \tau _G, \pi )$ . Then we have $W_G$ and ${\mathcal V}_{G, j}$ for $1\le j\le n_G$ as above.

We now verify conditions (i)–(iii) in Definition 3.1 as referenced in Definition 3.2. Denote by $V_1$ the set of all $v\in V$ satisfying $\pi _{g_1g_2}v=\pi _{g_1}\pi _{g_2}v$ for all $g_1, g_2\in A^{100+C_G}$ . Then $\mathrm {m}(V\setminus V_1)\le |A|^{2(100+C_G)}\tilde {\tau }_G$ . Also, denote by $V_2$ the set of $v\in V$ satisfying $\pi _g\pi _{g_1}v=\pi ^{\prime }_g\pi _{g_1}v$ for all $g\in A$ and $g_1\in A^{C_G}$ . Then $\mathrm {m}(V\setminus V_2)\le \tilde {\tau }_G|A|^{1+C_G}$ . Set $W_H'=W_G\cap V_1\cap V_2$ , and $W_H=W_H'\cup \sigma _{e_H}^{-1}(V\setminus \bigcup _{h\in S_H}\sigma _hW_H')$ . Then $\bigcup _{h\in S_H}\sigma _hW_H=V$ , verifying condition (ii) in Definition 3.1.

Note that

$$ \begin{align*} \mathrm{m}(W_H\setminus W_H')&\le 1-\mathrm{m}\bigg(\bigcup_{h\in S_H}\sigma_hW_H'\bigg)\\ &\le 1-\mathrm{m}\bigg(\bigcup_{g\in S_G}\pi^{\prime}_g W_H'\bigg)\\ &=1-\mathrm{m}\bigg(\bigcup_{g\in S_G}\pi_g W_H'\bigg)\\ &\le |S_G|(\mathrm{m}(V\setminus V_1)+\mathrm{m}(V\setminus V_2))\\ &\le |S_G|(\tilde{\tau}_G|A|^{2(100+C_G)}+ \tilde{\tau}_G|A|^{1+C_G})\\ &\le \delta_H. \end{align*} $$

Put ${\mathcal V}_{H, j}={\mathcal V}_{G, j}$ for all $1\le j\le n_G$ , and

$$ \begin{align*} {\mathcal V}_{H, n_H}=\bigcup_{h\in T_H}((W_H\setminus W_H')\cup \sigma_h(W_H\setminus W_H')\cup \sigma_h^{-1}(W_H\setminus W_H')). \end{align*} $$

Then

$$ \begin{align*} \mathrm{m} ({\mathcal V}_{H, n_H})\le (2|T_H|+1)\mathrm{m} (W_H\setminus W_H')\le 3|T_H|\delta_H, \end{align*} $$

and hence

$$ \begin{align*} \sum_{j=1}^{n_H} \Upsilon_H(S_{H, j})\mathrm{m}({\mathcal V}_{H, j})&=\Upsilon_H(T_H)\mathrm{m}({\mathcal V}_{H, n_H})+\sum_{j=1}^{n_G} \Upsilon_H(\kappa(S_{G, j}, X))\mathrm{m}({\mathcal V}_{G, j})\\ &=\Upsilon_H(T_H)\mathrm{m}({\mathcal V}_{H, n_H})+\frac{1}{2}\sum_{j=1}^{n_G} \Upsilon_G(S_{G, j})\mathrm{m}({\mathcal V}_{G, j})\\ &\le 3\Upsilon_H(T_H)|T_H|\delta_H+\tfrac12 \le 1, \end{align*} $$

verifying condition (i) in Definition 3.1. Let $h\in T_H$ and $w_1, w_2\in W_H$ with $\sigma _hw_1=w_2$ . If $w_1\not \in W_H'$ or $w_2\not \in W_H'$ , then $(w_1, w_2)$ is an $S_{H, n_H}$ -edge with both endpoints in ${\mathcal V}_{H, n_H}$ . We may thus assume that $w_1, w_2\in W_H'$ . Then

$$ \begin{align*} w_2=\sigma_hw_1=\pi^{\prime}_{\lambda(h, \varphi(w_1))}w_1=\pi_{\lambda(h, \varphi(w_1))}w_1\in \pi_{T_G}w_1 \end{align*} $$

and so $w_1$ and $w_2$ are connected by a path of length at most $C_G$ in which each edge is an $S_{G, j}$ -edge with both endpoints in ${\mathcal V}_{G, j}$ for some $1\le j\le n_G$ . It is easily checked that such an edge is also an $S_{H, j}$ -edge. This verifies condition (iii) in Definition 3.1.

3.7 Property sofic SC under bounded orbit equivalence

Proposition 3.18. Let $G\curvearrowright (X, \mu )$ and $H\curvearrowright (Y, \nu )$ be free p.m.p. actions which are boundedly orbit equivalent. Suppose that $G\curvearrowright (X, \mu )$ has property sofic SC. Then so does $H\curvearrowright (Y, \nu )$ .

To prove this proposition we may assume that $(X, \mu )=(Y, \nu )$ , the actions $G\curvearrowright X$ and $H\curvearrowright X$ are free, and the identity map of X provides a bounded orbit equivalence between the actions $G\curvearrowright X$ and $H\curvearrowright X$ . Let $\kappa : G\times X\to H$ and $\lambda : H\times X\to G$ be the associated cocyles.

For each $g\in G$ denote by ${\mathscr P}_g$ the finite Borel partition of X consisting of the sets $X_{g,t} := \{ x\in X : gx = tx \}$ for $t\in H$ , and likewise for $t\in H$ denote by ${\mathscr P}_t$ the finite Borel partition of X consisting of the sets $X_{g,t}$ for $g\in G$ . For every F in ${\mathcal F}(G)$ or ${\mathcal F}(H)$ , write ${}_F{\mathscr P}=\bigvee _{g\in F}{\mathscr P}_g$ .

The following is a specialization of [Reference Kerr and Li25, Lemma 4.2] to the case of bounded orbit equivalence, which permits a simplification of the statement.

Lemma 3.19. Let $F\in \overline {{\mathcal F}}(G)$ and set $L = \kappa (F^2 ,X) \in \overline {{\mathcal F}}(H)$ . Let $0<\tau <1$ and $0<\tau '\le \tau /(60|L|^2)$ . Let $\sigma : H\rightarrow \operatorname {\mathrm {Sym}}(V)$ be an $(L, \tau ')$ -approximation for H. Let $\varphi \in \operatorname {\mathrm {Hom}}_\mu ({}_{F^2}{\mathscr P}, L, \tau ', \sigma )$ . Let $\pi ': F^2\rightarrow V^V$ be such that

$$ \begin{align*} \pi^{\prime}_gv=\sigma_{\kappa(g, A)}v \end{align*} $$

for all $g\in F^2$ , $A\in {}_{F^2} {\mathscr P}$ and $v\in \varphi (A)$ . Then there is an $(F, \tau )$ -approximation $\pi : G\rightarrow \operatorname {\mathrm {Sym}}(V)$ for G such that $\rho _{\mathrm {Hamm}}(\pi _g, \pi ^{\prime }_g)\le \tau /5$ for all $g\in F^2$ .

Proof Proof of Proposition 3.18

Let $\Upsilon _H$ be a function ${\mathcal F}(H)\rightarrow [0, \infty )$ . Define a function $\Upsilon _G: {\mathcal F}(G)\rightarrow [0, \infty )$ by $\Upsilon _G(F)=2\Upsilon _H(\kappa (F, X))$ .

Since $G\curvearrowright (X, \mu )$ has property sofic SC, there exists an $S_G\in \overline {{\mathcal F}}(G)$ such that for any $T_G\in \overline {{\mathcal F}}(G)$ there are $C_G, n_G\in {\mathbb N}$ , $S_{G, 1}, \ldots , S_{G, n_G}\in \overline {{\mathcal F}}(G)$ , a finite Borel partition ${\mathscr C}_G$ of X, an $L_G\in \overline {{\mathcal F}}(G)$ , and $0<\tau _G<1$ such that, for any $(L_G, \tau _G)$ -approximation $\pi : G\rightarrow \operatorname {\mathrm {Sym}}(V)$ for G with $\operatorname {\mathrm {Hom}}_\mu ({\mathscr C}_G, L_G, \tau _G, \pi )\neq \emptyset $ , there are subsets $W_G$ and ${\mathcal V}_{G, j}$ of V for $1\le j\le n_G$ satisfying the following conditions:

  1. (i) $\sum _{j=1}^{n_G} \Upsilon _G(S_{G, j})\mathrm {m}({\mathcal V}_{G, j})\le 1$ ;

  2. (ii) $\bigcup _{g\in S_G}\pi _gW_G=V$ ;

  3. (iii) if $w_1, w_2\in W_G$ satisfy $\pi _gw_1=w_2$ for some $g\in T_G$ then $w_1$ and $w_2$ are connected by a path of length at most $C_G$ in which each edge is an $S_{G, j}$ -edge with both endpoints in ${\mathcal V}_{G, j}$ for some $1\le j\le n_G$ .

Set $S_H=\kappa (S_G, X)\in \overline {{\mathcal F}}(H)$ .

Let $T_H\in \overline {{\mathcal F}}(H)$ . Set $T_G=\lambda (T_H, X)\in \overline {{\mathcal F}}(G)$ . Then we have $C_G, n_G$ , $S_{G, j}$ for $1\le j\le n_G$ , ${\mathscr C}_G$ , $L_G$ , and $\tau _G$ as above. Set $C_H=C_G$ , $n_H=n_G+1$ , $S_{H, j}=\kappa (S_{G, j}, X)\in \overline {{\mathcal F}}(H)$ for $1\le j\le n_G$ , and $S_{H, n_H}=T_H\in \overline {{\mathcal F}}(H)$ . Take $0<\delta _H<1/(6\Upsilon _H(T_H)|T_H|)$ . Set $U=L_G\cup S_G\cup T_G\cup \bigcup _{j=1}^{n_G}S_{G, j}\in {\mathcal F}(G)$ , ${\mathscr C}_H=({\mathscr C}_G)_{L_G}\vee {}_{U^{2(100+C_G)}}{\mathscr P}\vee {}_{T_H}{\mathscr P}$ , $L_H=\kappa (U^{2(100+C_G)}, X)\in {\mathcal F}(H)$ , and

$$ \begin{align*} \tilde{\tau}_G &= \min\{\tau_G/4, \delta_H/(2|S_G|\cdot|U|^{2(100+C_G)})\}>0,\\ \tau_H &= \min\{\tilde{\tau}_G/(60|L_H|^2), \tau_G/(2|\kappa(L_G, X)|)\}>0. \end{align*} $$

Let $\sigma \!:\! H\rightarrow \operatorname {\mathrm {Sym}}(V)$ be an $(L_H, \tau _H)$ -approximation for H with $\operatorname {\mathrm {Hom}}_\mu ({\mathscr C}_H, L_H, \tau _H, \sigma )$ non-empty. Take $\varphi \in \operatorname {\mathrm {Hom}}_\mu ({\mathscr C}_H, L_H, \tau _H, \sigma )$ . Define $\pi ': U^{2(100+C_G)}\rightarrow V^V$ by

$$ \begin{align*} \pi^{\prime}_gv=\sigma_{\kappa(g, A)}v \end{align*} $$

for all $g\in U^{2(100+C_G)}$ , $A\in {\mathscr P}_g$ , and $v\in \varphi (A)$ . By Lemma 3.19 there is a $(U^{100+C_G}, \tilde {\tau }_G)$ - approximation $\pi : G\rightarrow \operatorname {\mathrm {Sym}}(V)$ for G such that $\rho _{\mathrm {Hamm}}(\pi _g, \pi ^{\prime }_g)\le \tilde {\tau }_G$ for all $g\in U^{100+C_G}$ .

Let $g\in L_G$ . We have

$$ \begin{align*} \sum_{A\in {\mathscr C}_G}\!\mathrm{m}(\pi_g\varphi(A)\Delta \varphi(gA))&\le \!\sum_{A\in {\mathscr C}_G}\!\mathrm{m}(\pi_g\varphi(A)\Delta \pi_g'\varphi(A))+\!\sum_{A\in {\mathscr C}_G}\!\mathrm{m}(\pi_g'\varphi(A)\Delta \varphi(gA))\\ &\le 2\rho_{\mathrm{Hamm}}(\pi_g, \pi_g')+\!\sum_{A\in {\mathscr C}_G}\!\sum_{B\in {\mathscr P}_g}\!\!\mathrm{m}(\pi_g'\varphi(A\cap B)\Delta \varphi(g(A\cap B))). \end{align*} $$

For any $A\in {\mathscr C}_G$ and $B\in {\mathscr P}_g$ , say $h=\kappa (g, B)\in L_H$ , we have $\pi _g'\varphi (A\cap B)=\sigma _h\varphi (A\cap B)$ and $\varphi (g(A\cap B))=\varphi (h(A\cap B))$ , whence

$$ \begin{align*} \sum_{A\in {\mathscr C}_G}\mathrm{m}(\pi_g'\varphi(A\cap B)\Delta \varphi(g(A\cap B)))=\sum_{A\in {\mathscr C}_G}\mathrm{m}(\sigma_h\varphi(A\cap B)\Delta \varphi(h(A\cap B)))\le \tau_H. \end{align*} $$

Therefore

$$ \begin{align*} \sum_{A\in {\mathscr C}_G}\!\mathrm{m}(\pi_g\varphi(A)\Delta \varphi(gA))&\le 2\rho_{\mathrm{Hamm}}(\pi_g, \pi_g')+\!\!\sum_{B\in {\mathscr P}_g}\!\sum_{A\in {\mathscr C}_G}\!\mathrm{m}(\pi_g'\varphi(A\cap B)\Delta \varphi(g(A\cap B)))\\ &\le 2\tilde{\tau}_G+\sum_{B\in {\mathscr P}_g}\tau_H\\ &\le \frac{\tau_G}{2} + |\kappa(g, X)|\tau_H\le \tau_G. \end{align*} $$

We also have

$$ \begin{align*} \sum_{A\in ({\mathscr C}_G)_{L_G}}|\mathrm{m}(\varphi(A))-\mu(A)|\le \sum_{B\in {\mathscr C}_H}|\mathrm{m}(\varphi(B))-\mu(B)|\le \tau_H\le \tau_G. \end{align*} $$

Therefore $\varphi \in \operatorname {\mathrm {Hom}}_\mu ({\mathscr C}_G, L_G, \tau _G, \pi )$ . Then we have $W_G$ and ${\mathcal V}_{G, j}$ for $1\le j\le n_G$ as above.

We now verify conditions (i)–(iii) in Definition 3.1 as referenced in Definition 3.3. Denote by $V_1$ the set of $v\in V$ satisfying $\pi _{g_1g_2}v=\pi _{g_1}\pi _{g_2}v$ for all $g_1, g_2\in U^{100+C_G}$ . Then $\mathrm {m}(V\setminus V_1)\le \tilde {\tau }_G|U|^{2(100+C_G)}$ . Also denote by $V_2$ the set of $v\in V$ satisfying $\pi _g\pi _{g_1}v=\pi ^{\prime }_g\pi _{g_1}v$ for all $g\in U$ and $g_1\in U^{C_G}$ . Then $\mathrm {m}(V\setminus V_2)\le \tilde {\tau }_G|U|^{1+C_G}$ . Set $W_H'=W_G\cap V_1\cap V_2$ , and $W_H=W_H'\cup \sigma _{e_H}^{-1}(V\setminus \bigcup _{h\in S_H}\sigma _hW_H')$ . Then $\bigcup _{h\in S_H}\sigma _hW_H=V$ , verifying condition (ii) in Definition 3.1. Note that

$$ \begin{align*} \mathrm{m}(W_H\setminus W_H')&\le 1-\mathrm{m}\bigg(\bigcup_{h\in S_H}\sigma_hW_H'\bigg)\\ &\le 1-\mathrm{m}\bigg(\bigcup_{g\in S_G}\pi^{\prime}_g W_H'\bigg)\\ &=1-\mathrm{m}\bigg(\bigcup_{g\in S_G}\pi_g W_H'\bigg)\\ &\le |S_G|(\mathrm{m}(V\setminus V_1)+\mathrm{m}(V\setminus V_2))\\ &\le |S_G|(\tilde{\tau}_G|U|^{2(100+C_G)}+ \tilde{\tau}_G|U|^{1+C_G})\le \delta_H. \end{align*} $$

Put ${\mathcal V}_{H, j}={\mathcal V}_{G, j}$ for all $1\le j\le n_G$ , and

$$ \begin{align*} {\mathcal V}_{H, n_H}=\bigcup_{h\in T_H}((W_H\setminus W_H')\cup \sigma_h(W_H\setminus W_H')\cup \sigma_h^{-1}(W_H\setminus W_H')). \end{align*} $$

Then

$$ \begin{align*} \mathrm{m} ({\mathcal V}_{H, n_H})\le (2|T_H|+1)\mathrm{m} (W_H\setminus W_H')\le 3|T_H|\delta_H, \end{align*} $$

and hence

$$ \begin{align*} \sum_{j=1}^{n_H} \Upsilon_H(S_{H, j})\mathrm{m}({\mathcal V}_{H, j})&=\Upsilon_H(T_H)\mathrm{m}({\mathcal V}_{H, n_H})+\sum_{j=1}^{n_G} \Upsilon_H(\kappa(S_{G, j}, X))\mathrm{m}({\mathcal V}_{G, j})\\ &=\Upsilon_H(T_H)\mathrm{m}({\mathcal V}_{H, n_H})+\frac{1}{2}\sum_{j=1}^{n_G} \Upsilon_G(S_{G, j})\mathrm{m}({\mathcal V}_{G, j})\\ &\le 3\Upsilon_H(T_H)|T_H|\delta_H+\tfrac12 \le 1, \end{align*} $$

verifying condition (i) in Definition 3.1. Let $h\in T_H$ and $w_1, w_2\in W_H$ with $\sigma _hw_1=w_2$ . If $w_1\not \in W_H'$ or $w_2\not \in W_H'$ , then $(w_1, w_2)$ is an $S_{H, n_H}$ -edge with both endpoints in ${\mathcal V}_{H, n_H}$ . Thus we may assume that $w_1, w_2\in W_H'$ . Then $w_1\in \varphi (A)$ for some $A\in {\mathscr P}_h$ . Set $g=\lambda (h, A)\in T_G$ . Then

$$ \begin{align*} w_2=\sigma_hw_1=\pi^{\prime}_gw_1=\pi_gw_1, \end{align*} $$

and so $w_1$ and $w_2$ are connected by a path of length at most $C_G$ in which each edge is an $S_{G, j}$ -edge with both endpoints in ${\mathcal V}_{G, j}$ for some $1\le j\le n_G$ . It is easily checked that such an edge is also an $S_{H, j}$ -edge. This verifies condition (iii) in Definition 3.1.

4 Topological entropy and continuous orbit equivalence

Our energies in this section will be invested in the proof of Theorem 4.1, which in conjunction with Theorem 3.12 and Proposition 3.15 yields Theorem C.

Theorem 4.1. Let $G\curvearrowright X$ and $H\curvearrowright Y$ be topologically free continuous actions on compact metrizable spaces, and suppose that they are continuously orbit equivalent. Let ${\mathscr S}$ be a collection of sofic approximations for G, and suppose that the action $G\curvearrowright X$ has property ${\mathscr S}$ -SC. Let $\Pi $ be a sofic approximation sequence for G in ${\mathscr S}$ . Then

$$ \begin{align*} h (H\curvearrowright Y)\ge h_\Pi (G\curvearrowright X). \end{align*} $$

For the purpose of establishing the theorem we may assume, by conjugating the H-action by a continuous orbit equivalence, that $Y=X$ and that the identity map on X is an orbit equivalence between the two actions. As usual we write $\kappa $ and $\lambda $ , respectively, for the cocycle maps $G\times X\rightarrow H$ and $H\times X \rightarrow G$ . As in §3.6, we take a dense $G_\delta $ subset $X_0$ of X such that $X_0$ is $G*H$ -invariant and that both G and H act freely on $X_0$ .

Fix a compatible metric d on X which gives X diameter no bigger than $1$ . For each $t\in G$ (respectively, $t\in H$ ) we can find an $\eta _t>0$ such that for any $x, y\in X$ with $d(x, y)\le \eta _t$ we have $\kappa (t, x)=\kappa (t, y)$ (respectively, $\lambda (t, x)=\lambda (t, y)$ ), and for a non-empty finite subset L of G or H we set $\eta _L=\min _{t\in L}\eta _t>0$ .

Lemma 4.2. Let $L\in \overline {{\mathcal F}}(H)$ and $0<\delta , \tau <1$ with $\tau <\delta ^2$ . Set $F=\lambda (L^2, X)\in \overline {{\mathcal F}}(G)$ and

$$ \begin{align*} \tau'=\min\{\eta_{L^2}\tau^{1/2}/(8|F|)^{1/2}, \tau/(22|F|^2)\}>0. \end{align*} $$

Let $\delta _1>0$ be such that $(\tau +7\delta _1)^{1/2}\le \delta $ . Let $\pi : G\rightarrow \operatorname {\mathrm {Sym}}(V)$ be an $(F, \tau ')$ -approximation for G. Suppose that $S\in \overline {{\mathcal F}}(G)$ and that W is a subset of V satisfying the following conditions:

  1. (i) $\pi _{g^{-1}}\pi _gw=w$ for all $w\in W$ and $g\in S$ ;

  2. (ii) $\pi _g\pi _a\pi _h w=\pi _{gah} w$ for all $g, h\in S$ , $a\in \lambda (L, X)$ , and $w\in W$ ;

  3. (iii) $\mathrm {m} ( \bigcup _{g\in S}\pi _gW ) \ge 1-\delta _1$ .

Take $0<\delta _2\le \eta _{S\cup \lambda (L, X)}$ such that for any $x, y\in X$ with $d(x, y)\le \delta _2$ one has $\max _{t\in \kappa (S, X)}d(tx, ty)\le \delta _1$ . Set

$$ \begin{align*} \delta'=\delta_1^{1/2}\delta_2/(|S|^{1/2}|S\lambda(L, X)S|^{1/2})>0. \end{align*} $$

Let $\varphi _0$ be a map in $\operatorname {\mathrm {Map}}_d(F, \tau ', \pi )\cap \operatorname {\mathrm {Map}}_d(S\lambda (L, X)S, \delta ', \pi )$ with $\varphi _0(V)\subseteq X_0$ and $\varphi $ a map in $\operatorname {\mathrm {Map}}_d(S\lambda (L, X)S, \delta ', \pi )$ such that

$$ \begin{align*} \kappa(g, \varphi_0(w))=\kappa(g, \varphi(w)) \end{align*} $$

for all $w\in W$ and $g\in S\lambda (L, X)S$ satisfying $\pi _gw\in W$ . Let $\sigma : H\rightarrow \operatorname {\mathrm {Sym}}(V)$ be a map such that $\rho _{\mathrm {Hamm}}(\sigma _t, \sigma ^{\prime }_t)\le \tau $ for all $t\in L$ , where $\sigma ': H\rightarrow V^V$ is given by

$$ \begin{align*} \sigma^{\prime}_tv=\pi_{\lambda(t, \varphi_0(v))}v \end{align*} $$

for all $t\in H$ and $v\in V$ . Take $\tilde {\varphi }: V\rightarrow X$ such that $\tilde {\varphi }=\varphi $ on W and such that for each $v\in \bigcup _{g\in S}\pi _gW$ one has

$$ \begin{align*} \tilde{\varphi}(v)=\kappa(g, \varphi_0(w))\varphi(w) \end{align*} $$

for some $g\in S$ and $w\in W$ with $\pi _gw=v$ . Then $\tilde {\varphi }\in \operatorname {\mathrm {Map}}_d(L, \delta , \sigma )$ .

Proof. For each $t\in H$ set $V_t=\{v\in V: \sigma _tv=\sigma ^{\prime }_tv\}$ . Then $\mathrm {m} (V_t )\ge 1-\tau $ for all $t\in L$ .

Denote by $V_\varphi $ the set of all $v\in V$ satisfying $d(g\varphi (v), \varphi (\pi _gv))\le \delta _2$ for all $g\in S\lambda (L, X)S$ . Then

$$ \begin{align*} \mathrm{m} (V\setminus V_\varphi )\le |S\lambda(L, X)S|\bigg(\frac{\delta'}{\delta_2}\bigg)^2 = \frac{\delta_1}{|S|}. \end{align*} $$

We define $V_{\varphi _0}$ in the same way, and get $\mathrm {m} (V\setminus V_{\varphi _0} )\le \delta _1/|S|$ . Set $W'=W\cap V_\varphi \cap V_{\varphi _0}$ and $V'=(\bigcup _{g\in S}\pi _gW)\setminus (\bigcup _{g\in S}\pi _g(V\setminus (V_\varphi \cap V_{\varphi _0})))$ . Then

$$ \begin{align*} \mathrm{m} (V' )\ge \mathrm{m}\bigg(\bigcup_{g\in S}\pi_gW\bigg)- |S|\cdot \mathrm{m} (V\setminus V_\varphi )-|S|\cdot \mathrm{m} (V\setminus V_{\varphi_0})\ge 1-3\delta_1. \end{align*} $$

Let $t\in L$ , $v_1\in V_t\cap V'$ , and $v_2\in V'$ be such that $\sigma _tv_1=v_2$ . Then we can find some $g_1,g_2\in S$ and $w_1, w_2\in W$ such that $\pi _{g_j}w_j=v_j$ and $\tilde {\varphi }(v_j)=\kappa (g_j, \varphi _0(w_j))\varphi (w_j)$ for $j=1, 2$ . Since $v_j\in V'$ , we actually have $w_j\in W'$ . We also have

$$ \begin{align*} w_2=\pi_{g_2^{-1}}v_2 &=\pi_{g_2^{-1}}\sigma_tv_1\\ &=\pi_{g_2^{-1}}\sigma^{\prime}_tv_1\\ &=\pi_{g_2^{-1}}\pi_{\lambda(t, \varphi_0(v_1))}v_1\\ &=\pi_{g_2^{-1}}\pi_{\lambda(t, \varphi_0(v_1))}\pi_{g_1}w_1\\ &=\pi_{g_2^{-1}\lambda(t, \varphi_0(v_1))g_1}w_1. \end{align*} $$

Observe that

$$ \begin{align*} d(g_1\varphi_0(w_1), \varphi_0(v_1))=d(g_1\varphi_0(w_1), \varphi_0(\pi_{g_1}w_1))\le \delta_2\le \eta_{\lambda(L, X)} \end{align*} $$

and

$$ \begin{align*}&d(\varphi_0(w_2), g_2^{-1}\lambda(t, \varphi_0(v_1))g_1\varphi_0(w_1))\\ & \quad = d(\varphi_0(\pi_{g_2^{-1}\lambda(t, \varphi_0(v_1))g_1}w_1), g_2^{-1}\lambda(t, \varphi_0(v_1))g_1\varphi_0(w_1))\le \delta_2\le \eta_S, \end{align*} $$

and hence

$$ \begin{align*} \kappa(\lambda(t, \varphi_0(v_1)), g_1\varphi_0(w_1))=\kappa(\lambda(t, \varphi_0(v_1)), \varphi_0(v_1))=t \end{align*} $$

and

$$ \begin{align*} \kappa(g_2^{-1}, \lambda(t, \varphi_0(v_1))g_1\varphi_0(w_1))=\kappa(g_2, g_2^{-1}\lambda(t, \varphi_0(v_1))g_1\varphi_0(w_1))^{-1}=\kappa(g_2, \varphi_0(w_2))^{-1}. \end{align*} $$

Therefore

$$ \begin{align*} &\kappa(g_2^{-1}\lambda(t, \varphi_0(v_1))g_1, \varphi_0(w_1))\\ &\quad=\kappa(g_2^{-1}, \lambda(t, \varphi_0(v_1))g_1\varphi_0(w_1))\kappa(\lambda(t, \varphi_0(v_1)), g_1\varphi_0(w_1))\kappa(g_1, \varphi_0(w_1))\\ &\quad=\kappa(g_2, \varphi_0(w_2))^{-1}t\kappa(g_1, \varphi_0(w_1)). \end{align*} $$

We then get

$$ \begin{align*} \kappa(g_2, \varphi_0(w_2))^{-1}\tilde{\varphi}(v_2)&=\varphi(w_2)\\ &\approx_{\delta_2} g_2^{-1}\lambda(t, \varphi_0(v_1))g_1\varphi(w_1)\\ &=\kappa(g_2^{-1}\lambda(t, \varphi_0(v_1))g_1, \varphi(w_1))\varphi(w_1)\\ &=\kappa(g_2^{-1}\lambda(t, \varphi_0(v_1))g_1, \varphi_0(w_1))\varphi(w_1)\\ &=\kappa(g_2, \varphi_0(w_2))^{-1}t\kappa(g_1, \varphi_0(w_1))\varphi(w_1)\\ &=\kappa(g_2, \varphi_0(w_2))^{-1}t\tilde{\varphi}(v_1), \end{align*} $$

and consequently $d(\tilde {\varphi }(v_2), t\tilde {\varphi }(v_1))\le \delta _1$ . We conclude that

$$ \begin{align*} d_2(t\tilde{\varphi}, \tilde{\varphi}\sigma_t)\le (\tau+6\delta_1+\delta_1^2)^{1/2} \le (\tau+7\delta_1)^{1/2}\le \delta \end{align*} $$

and hence that $\tilde {\varphi }\in \operatorname {\mathrm {Map}}_d(L, \delta , \sigma )$ .

Proof Proof of Theorem 4.1

Let $\Pi = \{ \pi _k : G\to \operatorname {\mathrm {Sym}} (V_k ) \}_{k=1}^\infty $ be a sofic approximation sequence in ${\mathscr S}$ with $h_\Pi (G\curvearrowright X)\ge 0$ . Let $\varepsilon>0$ . To establish the theorem it is enough to show the existence of a sofic approximation sequence $\Sigma $ for H such that $h_\Sigma (H\curvearrowright Y)\ge h_{\Pi , 2}^\varepsilon (G\curvearrowright X)-2\varepsilon $ .

For each $F\in {\mathcal F}(G)$ , since $\kappa : G\times X\rightarrow H$ is continuous there exists a finite clopen partition ${}_F {\mathscr P}$ of X such that for every $g\in F$ the map $x\mapsto \kappa (g,x)$ is constant on each member of ${}_F {\mathscr P}$ . Define $\Upsilon : {\mathcal F}(G)\rightarrow [0, \infty )$ by $\Upsilon (F)=(2/\varepsilon )\log |{}_F {\mathscr P} |$ .

Take a decreasing sequence $1>\delta _1>\delta _2>\cdots $ converging to $0$ . Take also a decreasing sequence $1>\tau _1>\tau _2>\cdots >0$ with $\tau _k^2<\delta _k$ for all k. Choose an increasing sequence $\{L_k\}$ in $\overline {{\mathcal F}}(H)$ with union H.

For each $k\in {\mathbb N}$ , set $F_k=\lambda (L_k^2, X)\subseteq G$ and $T_k'=\lambda (L_k, X)\subseteq F_k$ .

Since $G\curvearrowright X$ has property ${\mathscr S}$ -SC, there is some $S\in \overline {{\mathcal F}}(G)$ such that for each $k\in {\mathbb N}$ , there are $C_k, n_k\in {\mathbb N}$ , $S_{k, 1}, \ldots , S_{k, n_k}\in \overline {{\mathcal F}}(G)$ , $F^\sharp _k\in {\mathcal F}(G)$ , and $\delta ^\sharp _k>0$ such that for any good enough sofic approximation $\pi : G\rightarrow \operatorname {\mathrm {Sym}}(V)$ in ${\mathscr S}$ with $\operatorname {\mathrm {Map}}_d(F^\sharp _k, \delta ^\sharp _k, \pi )\neq \emptyset $ there are subsets $W'$ and ${\mathcal V}_j$ of V for $1\le j\le n_k$ satisfying the following conditions:

  1. (i) $\sum _{j=1}^{n_k} \Upsilon (S_{k,j})\mathrm {m}({\mathcal V}_j)\le 1$ ;

  2. (ii) $\bigcup _{g\in S}\pi _gW'=V$ ;

  3. (iii) if $w_1, w_2\in W'$ satisfy $\pi _gw_1=w_2$ for some $g\in T_k := ST_k'S\in \overline {{\mathcal F}}(G)$ then $w_1$ and $w_2$ are connected by a path of length at most $C_k$ in which each edge is an $S_{k, j}$ -edge with both endpoints in ${\mathcal V}_j$ for some $1\le j\le n_k$ .

Take $\varepsilon '>0$ such that for any $x, y\in X$ with $d(x, y)\le \varepsilon '$ one has $d(gx, gy)<\varepsilon /8$ for every $g\in S$ .

Fix $k\in {\mathbb N}$ . Set

$$ \begin{align*} \tau_k'=\min\{\eta_{L_k^2}\tau_k^{1/2}/(8|F_k|)^{1/2}, \tau_k/(22|F_k|^2)\}>0. \end{align*} $$

Let $0<\delta _{k, 1}<1/2$ be such that $(\tau _k+7\delta _{k, 1})^{1/2}\le \delta _k$ and $((\varepsilon /4)^2+\delta _{k, 1})^{1/2}<\varepsilon /2$ . Take $0<\delta _{k, 2}\le \eta _{T_k}$ such that for any $x, y\in X$ with $d(x, y)\le \! \delta _{k, 2}$ one has $\max _{t\in \kappa (S, X)}d(tx, ty) \le \delta _{k, 1}$ . Set $\delta _k'=\delta _{k, 1}^{1/2}\delta _{k, 2}/(|S|^{1/2}|T_k|^{1/2})>0$ and $\eta _k=\eta _{\bigcup _{j=1}^{n_k}S_{k, j}}$ . By Stirling’s formula there is some $0<\gamma _k<\delta _{k, 1}/(3|S|)$ such that for any non-empty finite set V the number of subsets of V with cardinality no bigger than $\gamma _k|V|$ is at most $e^{\varepsilon |V|/2}$ . Set $S_k=(\bigcup _{j=1}^{n_k}S_{k, j})^{C_k}\in {\mathcal F}(G)$ and $\delta _k''=\min \{\delta _k', \min \{\eta _k, \varepsilon /16\} (\gamma _k/|S_k\cup S|)^{1/2}, \tau _k'\}>0$ .

Take an $m_k\ge k$ large enough so that

$$ \begin{align*} &\frac{1}{|V_{m_k}|} \log N_{\varepsilon} (\operatorname{\mathrm{Map}}_d(T_k\cup S_k\cup F_k\cup F^\sharp_k, \min\{\delta_k''/2, \delta^\sharp_k\}, \pi_{m_k} ), d_2 )\\&\quad \ge \max\{0, h^{\varepsilon}_{\Pi, 2}(G\curvearrowright X)-\varepsilon\} \end{align*} $$

and so that $\pi _{m_k}: G\rightarrow \operatorname {\mathrm {Sym}}(V_{m_k})$ is an $(F_k, \tau _k')$ -approximation for G and also a good enough sofic approximation for G to guarantee the existence of $W'$ and ${\mathcal V}_1, \ldots , {\mathcal V}_{n_k}$ as above. Denote by $\tilde {V}_{m_k}$ the set of all $w\in V_{m_k}$ satisfying

  1. (iv) $\pi _{m_k, e_G}w=w$ ,

  2. (v) $\pi _{m_k, g^{-1}}\pi _{m_k, g}w=w$ for all $g\in S$ ,

  3. (vi) $\pi _{m_k, g}\pi _{m_k, a}\pi _{m_k, h}w=\pi _{m_k, gah}w$ for all $g, h\in S$ and $a\in T_k'$ ,

  4. (vii) $\pi _{m_k, gh}w=\pi _{m_k, g}\pi _{m_k, h}w$ for all $g, h\in S_k$ ,

  5. (viii) $\pi _{m_k, g}w\neq \pi _{m_k, h}w$ for all distinct $g, h$ in $T_k\cup S_k$ .

Taking $m_k$ sufficiently large, we may assume that $\mathrm {m}(\tilde {V}_{m_k})\ge 1-\delta _{k, 1}/(3|S|)$ .

Take a $(d_2, \varepsilon )$ -separated subset $\Phi $ of $\operatorname {\mathrm {Map}}_d(T_k\cup S_k\cup F_k, \delta _k''/2, \pi _{m_k} )$ with maximum cardinality. Since $X_0$ is dense in X, we may perturb each element of $\Phi $ to obtain a $(d_2, \varepsilon /2)$ -separated subset $\Phi _1$ of $\operatorname {\mathrm {Map}}_d(T_k\cup S_k\cup F_k, \delta _k'', \pi _{m_k} )$ with

$$ \begin{align*} |\Phi_1|=|\Phi|=N_{\varepsilon} (\operatorname{\mathrm{Map}}_d(T_k\cup S_k\cup F_k, \delta_k''/2, \pi_{m_k} ), d_2 ) \end{align*} $$

such that $\varphi (V_{m_k})\subseteq X_0$ for all $\varphi \in \Phi _1$ .

For each $\psi \in \operatorname {\mathrm {Map}}_d(T_k\cup S_k\cup F_k, \delta _k'', \pi _{m_k} )$ , using the fact that $\delta _k''\le \min \{\eta _k, \varepsilon /16\} \times (\gamma _k/|S_k\cup S|)^{1/2}$ , we have $\mathrm {m}(V_{\psi })\ge 1-\gamma _k$ where

$$ \begin{align*} V_\psi:=\{v\in V_{m_k}: d(g\psi(v), \psi(\pi_{m_k, g}v))\le \min\{\eta_k, \varepsilon/16\} \mbox{ for all } g\in S_k\cup S\}. \end{align*} $$

Thus there is a subset $\Phi _2$ of $\Phi _1$ such that $V_\varphi $ is the same for all $\varphi \in \Phi _2$ and

$$ \begin{align*} |\Phi_1|\le |\Phi_2|e^{\varepsilon |V_{m_k}|/2}. \end{align*} $$

Set $W=W'\cap \tilde {V}_{m_k}\cap V_\varphi \subseteq V_{m_k}$ for $\varphi \in \Phi _2$ . Then

$$ \begin{align*} &\mathrm{m}\bigg(\bigcup_{g\in S}\pi_{m_k, g}W\bigg)\\ &\quad\ge \mathrm{m}\bigg(\bigcup_{g\in S}\pi_{m_k, g}W'\bigg)-\mathrm{m}\bigg(\bigcup_{g\in S}\pi_{m_k, g}(V\setminus \tilde{V}_{m_k})\bigg)-\mathrm{m}\bigg(\bigcup_{g\in S}\pi_{m_k, g}(V\setminus V_\varphi)\bigg)\\ &\quad\ge 1-\frac{\delta_{k, 1}}{3}-\gamma_k|S|\ge 1-\delta_{k, 1}. \end{align*} $$

For each $\psi : V_{m_k}\rightarrow X$ , define $\Theta (\psi )\in \prod _{j=1}^{n_k}H^{S_{k, j}\times {\mathcal V}_j}$ by $\Theta (\psi )(g_j, v_j)=\kappa (g_j, \psi (v_j))$ for $1\le j\le n_k$ and $(g_j, v_j)\in S_{k, j}\times {\mathcal V}_j$ . Then

$$ \begin{align*} |\Theta(X^{V_{m_k}})|\le \prod_{j=1}^{n_k}|{}_{S_{k, j}}{\mathscr P}|^{|{\mathcal V}_j|}=\prod_{j=1}^{n_k}e^{(\varepsilon/2)\Upsilon(S_{k, j})|{\mathcal V}_j|}=e^{(\varepsilon/2)\sum_{j=1}^{n_k}\Upsilon(S_{k, j})|{\mathcal V}_j|}\le e^{\varepsilon |V_{m_k}|/2}. \end{align*} $$

Thus we can find a subset $\Phi _3$ of $\Phi _2$ such that $\Theta (\varphi )$ is the same for all $\varphi \in \Phi _3$ and

$$ \begin{align*} |\Phi_2|\le |\Phi_3|e^{\varepsilon |V_{m_k}|/2}. \end{align*} $$

We claim that for any $g\in T_k$ and $w_1, w_2\in W$ with $\pi _{m_k, g}w_1=w_2$ , the element $\kappa (g, \varphi (w_1))\in H$ is the same for all $\varphi \in \Phi _3$ . If $w_1=w_2$ , then $g=e_G$ and hence $\kappa (g, \varphi (w_1))=e_H$ for all $\varphi \in \Phi _3$ . Thus we may assume that $w_1\neq w_2$ . We can find $l\le C_k$ , $g_1, \ldots , g_l\in G$ , $w_1=w_1', w_2', \ldots , w_{l+1}'=w_2$ in $V_{m_k}$ such that for each $1\le i\le l$ one has $\pi _{m_k, g_i}w_i'=w_{i+1}'$ , $g_i\in S_{k, j_i}$ and $w_i', w_{i+1}'\in {\mathcal V}_{j_i}$ for some $1\le j_i\le n_k$ . Since $w_1'\in W\subseteq \tilde {V}_{m_k}$ , we have

$$ \begin{align*} \pi_{m_k, g_ig_{i-1}\cdots g_1}w_1'=\pi_{m_k, g_i}\pi_{m_k, g_{i-1}}\cdots \pi_{m_k, g_1}w_1'=w_{i+1}' \end{align*} $$

for all $1\le i\le l$ . In particular, $\pi _{m_k, g_lg_{l-1}\cdots g_1}w_1'=w_{l+1}'=\pi _{m_k, g}w_1'$ , and hence

$$ \begin{align*} g_lg_{l-1}\cdots g_1=g. \end{align*} $$

Note that $w_1'\in W\subseteq V_\varphi $ for all $\varphi \in \Phi _3\subseteq \Phi _2$ . For each $0\le i\le l-1$ and $\varphi \in \Phi _3$ , we have $g_ig_{i-1}\cdots g_1\in S_k$ , and hence $d(g_ig_{i-1}\cdots g_1\varphi (w_1'), \varphi (\pi _{m_k, g_ig_{i-1}\cdots g_1}w_1'))\le \eta _k$ , which implies that

$$ \begin{align*} \kappa(g_{i+1}, g_ig_{i-1}\cdots g_1\varphi(w_1'))=\kappa(g_{i+1}, \varphi(\pi_{m_k, g_ig_{i-1}\cdots g_1}w_1')). \end{align*} $$

Then

$$ \begin{align*} \kappa(g, \varphi(w_1))=\kappa(g_lg_{l-1}\cdots g_1, \varphi(w_1')) &=\prod_{i=0}^{l-1}\kappa(g_{i+1}, g_ig_{i-1}\cdots g_1\varphi(w_1'))\\ &=\prod_{i=0}^{l-1}\kappa(g_{i+1}, \varphi(\pi_{m_k, g_ig_{i-1}\cdots g_1}w_1'))\\ &=\prod_{i=0}^{l-1}\kappa(g_{i+1}, \varphi(w_{i+1}'))\\ &=\prod_{i=0}^{l-1}\Theta(\varphi)(g_{i+1}, w_{i+1}') \end{align*} $$

is the same for all $\varphi \in \Phi _3$ . This proves our claim.

Fix one $\varphi _0\in \Phi _3$ . Define $\sigma _k': H\rightarrow V_{m_k}^{V_{m_k}}$ by

$$ \begin{align*} \sigma^{\prime}_{k,t}v=\pi_{\lambda(t, \varphi_0(v))}v \end{align*} $$

for all $t\in H$ and $v\in V_{m_k}$ . By Lemma 3.17 there is an $(L_k, \tau _k)$ -approximation $\sigma _k: H\rightarrow \operatorname {\mathrm {Sym}}(V_{m_k})$ for H such that $\rho _{\mathrm {Hamm}}(\sigma _{k, t}, \sigma ^{\prime }_{k, t})\le \tau _k$ for all $t\in L_k$ . For each $\varphi \in \Phi _3$ take a $\tilde {\varphi }: V_{m_k}\rightarrow X$ such that $\tilde {\varphi }=\varphi $ on W and such that for each $v\in \bigcup _{g\in S}\pi _{m_k, g}W$ one has

$$ \begin{align*} \tilde{\varphi}(v)=\kappa(g, \varphi_0(w))\varphi(w) \end{align*} $$

for some $g\in S$ and $w\in W$ with $\pi _{m_k, g}w=v$ . We may require that g and w depend only on v, and not on $\varphi \in \Phi _3$ . By Lemma 4.2 we have $\tilde {\varphi }\in \operatorname {\mathrm {Map}}_d(L_k, \delta _k, \sigma _k)$ .

Let $\varphi $ and $\psi $ be distinct elements in $\Phi _3$ . Since $d_2(\varphi , \psi )\ge \varepsilon /2> ((\varepsilon /4)^2+\delta _{k, 1})^{1/2}$ and $\mathrm {m}(\bigcup _{g\in S}\pi _{m_k, g}W)\ge 1-\delta _{k, 1}$ , we have $d(\varphi (v), \psi (v))>\varepsilon /4$ for some $v\in \bigcup _{g\in S}\pi _{m_k, g}W$ . Then $v=\pi _{m_k, g}w$ for some $g\in S$ and $w\in W$ such that $\tilde {\varphi }(v)=\kappa (g, \varphi _0(w))\varphi (w)$ and $\tilde {\psi }(v)=\kappa (g, \varphi _0(w))\psi (w)$ . Using the fact that $w\in W\subseteq V_{\varphi }=V_{\psi }$ , we have

$$ \begin{align*} &d(g\varphi(w), g\psi(w))\\ &\quad\ge d(\varphi(\pi_{m_k, g}w), \psi(\pi_{m_k, g}w))-d(\varphi(\pi_{m_k, g}w), g\varphi(w))-d(\psi(\pi_{m_k, g}w), g\psi(w))\\ &\quad\ge \frac{\varepsilon}{4}-\frac{\varepsilon}{16}-\frac{\varepsilon}{16}= \frac{\varepsilon}{8}. \end{align*} $$

From our choice of $\varepsilon '$ we get $d(\tilde {\varphi }(w), \tilde {\psi }(w))=d(\varphi (w), \psi (w))>\varepsilon '$ . Therefore $\tilde {\Phi }_3:=\{\tilde {\varphi }: \varphi \in \Phi _3\}$ is $(d_\infty , \varepsilon ')$ -separated and $|\tilde {\Phi }_3|=|\Phi _3|$ . Thus

$$ \begin{align*} \frac{1}{|V_{m_k}|}\log N_{\varepsilon'}(\operatorname{\mathrm{Map}}_d(L_k, \delta_k, \sigma_k), d_\infty)\ge \frac{1}{|V_{m_k}|}\log |\tilde{\Phi}_3| &= \frac{1}{|V_{m_k}|}\log |\Phi_3|\\ &\ge \frac{1}{|V_{m_k}|}\log |\Phi_1|-\varepsilon\\ &\ge h^{\varepsilon}_{\Pi, 2}(G\curvearrowright X)-2\varepsilon. \end{align*} $$

Now $\Sigma =\{\sigma _k\}_{k\in {\mathbb N}}$ is a sofic approximation sequence for H. For any finite set $L\subseteq H$ and $\delta>0$ , we have $L\subseteq L_k$ and $\delta>\delta _k$ for all large enough k, and hence

$$ \begin{align*} \varlimsup_{k\to \infty}\frac{1}{|V_{m_k}|}\log N_{\varepsilon'}(\operatorname{\mathrm{Map}}_d(L, \delta, \sigma_k), d_\infty)&\ge \varlimsup_{k\to \infty}\frac{1}{|V_{m_k}|}\log N_{\varepsilon'}(\operatorname{\mathrm{Map}}_d(L_k, \delta_k, \sigma_k), d_\infty)\\ &\ge h^{\varepsilon}_{\Pi, 2}(G\curvearrowright X)-2\varepsilon. \end{align*} $$

Taking infima over L and $\delta $ , we obtain

$$ \begin{align*} h_\Sigma(H\curvearrowright X)\ge h_{\Sigma, \infty}^{\varepsilon'}(H\curvearrowright X)\ge h^{\varepsilon}_{\Pi, 2}(G\curvearrowright X)-2\varepsilon.\\ \end{align*} $$

5 Measure entropy and bounded orbit equivalence

In this final section we establish Theorem 5.2, which in conjunction with Proposition 3.15 yields Theorem A.

For a general reference on the C $^*$ -algebra theory and terminology used in the following proof, see [Reference Murphy31].

Lemma 5.1. Let $G\curvearrowright (X, \mu )$ and $H\curvearrowright (Y, \nu )$ be orbit equivalent free p.m.p. actions and suppose that $H\curvearrowright (Y, \nu )$ is uniquely ergodic. Then there are a zero-dimensional compact metrizable space Z, a continuous action $G*H \curvearrowright Z$ , and a $G*H$ -invariant Borel probability measure $\mu _Z$ on Z of full support such that:

  1. (i) $G\curvearrowright (Z, \mu _Z)$ is measure conjugate to $G\curvearrowright (X, \mu )$ and $H\curvearrowright (Z, \mu _Z)$ is measure conjugate to $H\curvearrowright (Y, \nu )$ ;

  2. (ii) $H\curvearrowright Z$ is uniquely ergodic;

  3. (iii) there is a $G*H$ -invariant Borel subset $Z_0$ of Z with $\mu _Z(Z_0)=1$ such that $Gz=Hz$ for every $z\in Z_0$ .

If, furthermore, $G\curvearrowright (X, \mu )$ and $H\curvearrowright (Y, \nu )$ are boundedly orbit equivalent then we may demand that both $G\curvearrowright Z_0$ and $H\curvearrowright Z_0$ be free and that the cocycles $\kappa : G\times Z_0\rightarrow H$ and $\lambda : H\times Z_0\rightarrow G$ extend to continuous maps $G\times Z\rightarrow H$ and $H\times Z\rightarrow G$ , so that $G\curvearrowright Z$ and $H\curvearrowright Z$ are continuously orbit equivalent.

Proof. We may assume that $(X, \mu )=(Y, \nu )$ and that $Gx=Hx$ for every $x\in X$ . Denote by ${\mathscr B}$ the $\sigma $ -algebra of Borel subsets of X. Denote by $\varphi $ the mean $f\mapsto \int _X f\, d\mu $ on $L^\infty (X, \mu )$ .

Let V be a finite subset of ${\mathscr B}$ . We claim that for every $\varepsilon>0$ there is a finite subset W of ${\mathscr B}$ containing V such that for any mean $\psi $ on $L^\infty (X, \mu )$ satisfying $\psi (s1_A)=\psi (1_A)$ for all $s\in H$ and $A\in W$ one has $|\varphi (1_A)-\psi (1_A)|<\varepsilon $ for all $A\in V$ . Suppose to the contrary that for some $\varepsilon> 0$ and every finite subset W of ${\mathscr B}$ containing V there is a mean $\psi _W$ on $L^\infty (X, \mu )$ satisfying $\psi _W(s1_A)=\psi _W(1_A)$ for all $s\in H$ and $A\in W$ and $\max _{A\in V}|\varphi (1_A)-\psi _W(1_A)|\ge \varepsilon $ . Then any cluster point $\psi $ of the net $\{ \psi _W \}$ (with index directed by inclusion) is H-invariant and $\max _{A\in V}|\varphi (1_A)-\psi (1_A)|\ge \varepsilon $ . This contradicts the unique ergodicity of $H\curvearrowright (X, \mu )$ , thus verifying our claim.

For any countable subset V of ${\mathscr B}$ , writing V as the union of an increasing sequence $\{V_k\}_k$ of finite subsets of V and taking a sequence $\{\varepsilon _k\}_k$ of positive numbers tending to $0$ , we conclude from above that there is a countable subset W of ${\mathscr B}$ containing V such that for any mean $\psi $ on $L^\infty (X, \mu )$ satisfying $\psi (s1_A)=\psi (1_A)$ for all $s\in H$ and $A\in W$ one has $\varphi (1_A)=\psi (1_A)$ for all $A\in V$ .

For a given countable set ${\mathscr A}\subseteq {\mathscr B}$ , denote by ${\mathscr A\,}'$ the $G*H$ -invariant subalgebra of ${\mathscr B}$ generated by ${\mathscr A}$ , which is again countable. Take a countable subset ${\mathscr A}_1$ of ${\mathscr B}$ such that for any distinct $x, y\in X$ one has $1_A(x)\neq 1_A(y)$ for some $A\in {\mathscr A}_1$ . Inductively, having constructed a countable subset ${\mathscr A}_k$ of ${\mathscr B}$ , we take a countable subset ${\mathscr A}_{k+1}$ of ${\mathscr B}$ containing ${\mathscr A\,}^{\prime }_k$ such that for any mean $\psi $ on $L^\infty (X, \mu )$ satisfying $\psi (s1_A)=\psi (1_A)$ for all $s\in H$ and $A\in {\mathscr A}_{k+1}$ , one has $\varphi (1_A)=\psi (1_A)$ for all $A\in {\mathscr A\,}^{\prime }_k$ .

Now we put ${\mathscr A}=\bigcup _k{\mathscr A}_k$ . This is a countable $G*H$ -invariant subalgebra of ${\mathscr B}$ . For any mean $\psi $ on $L^\infty (X, \mu )$ satisfying $\psi (s1_A)=\psi (1_A)$ for all $s\in H$ and $A\in {\mathscr A}$ , one has $\varphi (1_A)=\psi (1_A)$ for all $A\in {\mathscr A}$ . Denote by ${\mathfrak A}$ the $G*H$ -invariant unital C $^*$ -subalgebra of $L^\infty (X, \mu )$ generated by the functions $1_A$ for $A\in {\mathscr A}$ . Then ${\mathfrak A}$ is the closure of the linear span of the functions $1_A$ for $A\in {\mathscr A}$ in $L^\infty (X, \mu )$ . Thus every state of ${\mathfrak A}$ is determined by its values on the functions $1_A$ for $A\in {\mathscr A}$ . Since every state of ${\mathfrak A}$ extends to a mean of $L^\infty (X, \mu )$ , we conclude that $\varphi |_{\mathfrak A}$ is the unique H-invariant state on ${\mathfrak A}$ .

Define a $G*H$ -action on $\{0, 1\}^{{\mathscr A}\times (G*H)}$ by $(sw)_{A,t} = w_{A,s^{-1} t}$ for $w\in \{0, 1\}^{{\mathscr A}\times (G*H)}$ , $A\in {\mathscr A}$ , and $s,t\in G*H$ , and consider the $G*H$ -equivariant Borel map $\pi : X\rightarrow \{0, 1\}^{{\mathscr A}\times (G*H)}$ given by $\pi (x)_{A, t}=1_A(t^{-1}x)=1_{tA}(x)$ for $x\in X$ , $A\in {\mathscr A}$ , and $t\in G*H$ . Since ${\mathscr A}_1\subseteq {\mathscr A}$ , the map $\pi $ is injective and hence is a Borel isomorphism from X to $\pi (X)$ [Reference Kechris20, Corollary 15.2]. Put $\mu _Z=\pi _*\mu $ and $Z=\operatorname {\mathrm {supp}}(\mu _Z)$ . Then Z is zero-dimensional and $\mu _Z$ is a $G*H$ -invariant Borel probability measure on Z of full support. Put $Z_0=\pi (X)\cap Z$ . Then $Z_0$ is $G*H$ -invariant with $\mu _Z(Z_0)=1$ , and $Gz=Hz$ for all $z\in Z_0$ . The pullback map $\pi ^*: C(Z)\rightarrow L^\infty (X, \mu )$ is a $G*H$ -equivariant $*$ -homomorphism. From the Stone–Weierstrass theorem we get $\pi ^*(C(Z))={\mathfrak A}$ . Since Z is the support of $\pi _*\mu $ , the map $\pi ^*$ is injective and hence is an isomorphism from $C(Z)$ to ${\mathfrak A}$ . Thus $C(Z)$ has a unique H-invariant state, which means that $H\curvearrowright Z$ is uniquely ergodic.

Now assume that $G\curvearrowright (X, \mu )$ and $H\curvearrowright (Y, \nu )$ are boundedly orbit equivalent. By passing to suitable invariant subsets we may assume that $G\curvearrowright X$ and $H\curvearrowright X$ are both genuinely free and that the cocycles $\kappa ': G\times X\rightarrow H$ and $\lambda ': H\times X\rightarrow G$ are both bounded. Adding more sets to ${\mathscr A}_1$ , we may assume that for every $t\in G$ (respectively, $t\in H$ ) there is a finite partition ${\mathscr P}$ of X contained in ${\mathscr A}_1$ such that $\kappa '$ (respectively, $\lambda '$ ) is constant on $\{t\}\times P$ for every $P\in {\mathscr P}$ . Then we can extend $\kappa $ (respectively, $\lambda $ ) continuously to $G\times Z\rightarrow H$ (respectively, $H\times Z\rightarrow G$ ).

Theorem 5.2. Let $G\curvearrowright (X,\mu )$ and $H\curvearrowright (Y,\nu )$ be free p.m.p. actions which are boundedly orbit equivalent. Let ${\mathscr S}$ be a collection of sofic approximations for G. Suppose that G has property ${\mathscr S}$ -SC and that the action $H\curvearrowright (Y,\nu )$ is uniquely ergodic. Let $\Pi $ be a sofic approximation sequence in ${\mathscr S}$ . Then

$$ \begin{align*} h_\nu (H\curvearrowright Y)\ge h_{\Pi,\mu} (G\curvearrowright X). \end{align*} $$

Proof. Combine Lemma 5.1, Theorem 4.1, and the variational principle [Reference Kerr and Li24, Theorem 10.35].

Acknowledgements

The first author was partially supported by NSF grant DMS-1800633 and was affiliated with Texas A&M University during the course of the work. Preliminary stages were carried out during his six-month stay at the ENS de Lyon in 2017–2018, during which time he held ENS and CNRS visiting professorships and was supported by Labex MILYON/ANR-10-LABX-0070. The second author was partially supported by NSF grants DMS-1600717 and DMS-1900746. We thank the referee for helpful comments and suggestions.

References

Alpeev, A.. The entropy of Gibbs measures on soficgroups. Zap. Nauchn. Sem. S.-Peterburg. Otdel. Mat. Inst. Steklov. (POMI) 436(2015), 3448.Google Scholar
Alpeev, A.. Random ordering formula for sofic and Rokhlin entropy of Gibbsmeasures. Preprint, 2017, arXiv:1705.08559.Google Scholar
Austin, T.. Behaviour of entropy under bounded and integrable orbitequivalence. Geom. Funct. Anal. 26 (2016),14831525.CrossRefGoogle Scholar
Belinskaya, R. M.. Partitions of Lebesgue space in trajectoriesdefined by ergodic automorphisms. Funct. Anal. Appl. 2 (1968),190199.CrossRefGoogle Scholar
Bowen, L.. Measure conjugacy invariants for actions of countablesofic groups. J. Amer. Math. Soc. 23 (2010),217245.CrossRefGoogle Scholar
Bowen, L.. Sofic entropy and amenable groups.Ergod. Th. & Dynam. Sys. 32 (2012),427466.CrossRefGoogle Scholar
Chung, N.-P. and Jiang, Y.. Continuous cocycle superrigidity for shifts and groups with one end.Math. Ann. 368 (2017), 11091132.CrossRefGoogle Scholar
Cohen, D. B.. Continuous cocycle superrigidity for the full shiftover a finitely generated torsion group. Int. Math. Res. Not. IMRN 2020(2020), 16101620.CrossRefGoogle Scholar
del Junco, A. and Rudolph, D. J.. Kakutani equivalence of ergodic ${\mathbb{Z}}^n$ actions. Ergod. Th. & Dynam. Sys. 4 (1984),89104.CrossRefGoogle Scholar
Dye, H. A.. On groups of measure preserving transformationsI. Amer. J. Math. 81 (1959),119159.CrossRefGoogle Scholar
Feldman, J.. New $K$ -automorphisms and a problem ofKakutani. Israel J. Math. 24 (1976),1638.CrossRefGoogle Scholar
Fieldsteel, A. and Friedman, N. A.. Restricted orbit changes of ergodic ${\mathbf{Z}}^d$ -actions to achieve mixing and completelypositive entropy. Ergod. Th. & Dynam. Sys. 6 (1986),505528.CrossRefGoogle Scholar
Gaboriau, D.. Coût des relations d’équivalenceet des groupes. Invent. Math. 139 (2000),4198.CrossRefGoogle Scholar
Hayes, B.. Fuglede–Kadison determinants and soficentropy. Geom. Funct. Anal. 26 (2016),520606.CrossRefGoogle Scholar
Hayes, B.. Polish models and sofic entropy.J. Inst. Math. Jussieu 17 (2018),241275.CrossRefGoogle Scholar
Hayes, B.. Relative entropy and the Pinsker product formula forsofic groups. Groups Geom. Dyn. 15 (2021),413463.CrossRefGoogle Scholar
Kammeyer, J. W. and Rudolph, D. J.. Restricted orbit equivalence for ergodic ${\mathbb{Z}}^d$ actionsI. Ergod. Th. & Dynam. Sys. 17 (1997),10831129.CrossRefGoogle Scholar
Kammeyer, J. W. and Rudolph, D. J.. Restricted Orbit Equivalence for Actions of Discrete Amenable Groups (Cambridge Tracts in Mathematics, 146). Cambridge University Press,Cambridge, 2002.CrossRefGoogle Scholar
Katok, A. B.. Monotone equivalence in ergodictheory. Izv. Akad. Nauk SSSR Ser. Mat. 41 (1977),104157.Google Scholar
Kechris, A. S.. Classical Descriptive Set Theory (Graduate Texts in Mathematics, 156). Springer, New York,1995.CrossRefGoogle Scholar
Kerr, D.. Sofic measure entropy via finitepartitions. Groups Geom. Dyn. 7 (2013),617632.CrossRefGoogle Scholar
Kerr, D. and Li, H.. Bernoulli actions and infinite entropy. Groups Geom.Dyn. 5 (2011), 663672.CrossRefGoogle Scholar
Kerr, D. and Li, H.. Soficity, amenability, and dynamical entropy. Amer. J.Math. 135 (2013), 721761.CrossRefGoogle Scholar
Kerr, D. and Li, H.. Ergodic Theory: Independence and Dichotomies.Springer, Cham, 2016.CrossRefGoogle Scholar
Kerr, D. and Li, H.. Entropy, Shannon orbit equivalence, and sparse connectivity.Math. Ann. 380 (2021), 14971562.CrossRefGoogle Scholar
Kolmogorov, A. N.. A new metric invariant of transient dynamicalsystems and automorphisms in Lebesgue spaces. Dokl. Akad. Nauk SSSR (N.S.) 119(1958), 861864.Google Scholar
Kolmogorov, A. N.. Entropy per unit time as a metric invariant ofautomorphisms. Dokl. Akad. Nauk SSSR (N.S.) 124 (1959),754755.Google Scholar
Li, X.. Continuous orbit equivalence rigidity.Ergod. Th. & Dynam. Sys. 38 (2018),15431563.CrossRefGoogle Scholar
Mann, A.. How Groups Grow (London Mathematical SocietyLecture Note Series, 395). Cambridge University Press, Cambridge,2012.Google Scholar
Meyerovitch, T.. Positive sofic entropy implies finitestabilizer. Entropy 18 (2016), 263.CrossRefGoogle Scholar
Murphy, G. J.. C*-Algebras and Operator Theory.Academic Press, San Diego, CA, 1990.Google Scholar
Ornstein, D.. Bernoulli shifts with the same entropy areisomorphic. Adv. Math. 4 (1970),337352.CrossRefGoogle Scholar
Ornstein, D. S., Rudolph, D. J. and Weiss, B..Equivalence of measure preserving transformations. Mem. Amer. Math. Soc. 37(1982), 262.Google Scholar
Ornstein, D. S. and Weiss, B.. Ergodic theory of amenable group actions. I. The Rohlin lemma.Bull. Amer. Math. Soc. (N.S.) 2 (1980),161164.CrossRefGoogle Scholar
Peterson, J. and Sinclair, T.. On cocycle superrigidity for Gaussian actions. Ergod. Th.& Dynam. Sys. 32 (2012), 249272.CrossRefGoogle Scholar
Popa, S.. On the superrigidity of malleable actions with spectralgap. J. Amer. Math. Soc. 21 (2008),9811000.CrossRefGoogle Scholar
Rudolph, D. J.. Restricted orbit equivalence.Mem. Amer. Math. Soc. 54 (1985), 323.Google Scholar
Rudolph, D. J. and Weiss, B.. Entropy and mixing for amenable group actions. Ann. of Math.(2) 151 (2000), 11191150.CrossRefGoogle Scholar
Schmidt, K.. Amenability, Kazhdan’s property T, strongergodicity and invariant means for ergodic group-actions. Ergod. Th. & Dynam. Sys. 1(1981), 223236.CrossRefGoogle Scholar
Seward, B.. Positive entropy actions of countable groups factoronto Bernoulli shifts. J. Amer. Math. Soc. 33 (2020),57101.CrossRefGoogle Scholar
Sinai, Y.. On the concept of entropy for a dynamicsystem. Dokl. Akad. Nauk SSSR (N.S.) 124 (1959),768771.Google Scholar
Vershik, A. M.. Approximation in measure theory. PhD Thesis,Leningrad University, 1973 (in Russian).Google Scholar
Vershik, A. M.. Theory of decreasing sequences of measurablepartitions. St. Petersburg Math. J. 6 (1995),705761.Google Scholar