A Short Proof of Bernoulli Disjointness via the Local Lemma
Anton Bernshteyn

TL;DR
This paper provides a concise, combinatorial proof that all minimal group actions are disjoint from Bernoulli shifts, utilizing the Lovász Local Lemma to unify the argument across all groups.
Contribution
It introduces a short, self-contained combinatorial proof of Bernoulli disjointness for all groups using the Lovász Local Lemma, simplifying previous complex proofs.
Findings
Unified proof applicable to all groups
Utilizes Lovász Local Lemma in dynamical systems
Simplifies previous complex arguments
Abstract
Recently, Glasner, Tsankov, Weiss, and Zucker showed that if is an infinite discrete group, then every minimal -flow is disjoint from the Bernoulli shift . Their proof is somewhat involved; in particular, it invokes separate arguments for different classes of groups. In this note, we give a short and self-contained proof of their result using purely combinatorial methods applicable to all groups at once. Our proof relies on the Lov\'{a}sz Local Lemma, an important tool in probabilistic combinatorics that has recently found several applications in the study of dynamical systems.
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A Short Proof of Bernoulli Disjointness via the
Local Lemma
Anton Bernshteyn
Department of Mathematical Sciences, Carnegie Mellon University, Pittsburgh, PA, 15213, USA
Abstract.
Recently, Glasner, Tsankov, Weiss, and Zucker showed that if is an infinite discrete group, then every minimal -flow is disjoint from the Bernoulli shift . Their proof is somewhat involved; in particular, it invokes separate arguments for different classes of groups. In this note, we give a short and self-contained proof of their result using purely combinatorial methods applicable to all groups at once. Our proof relies on the Lovász Local Lemma, an important tool in probabilistic combinatorics that has recently found several applications in the study of dynamical systems.
††2010 Mathematics Subject Classification: Primary 37B05, 37B10; Secondary 05D40.††Key words and phrases: disjointness, minimal flows, Bernoulli flow, Lovász Local Lemma.
1. Introduction
Throughout, denotes an infinite discrete (but not necessarily countable) group. All topological spaces in this paper are assumed to be Hausdorff. A -flow is a nonempty compact space equipped with a continuous action . A subflow of a -flow is a nonempty closed -invariant subset . A -flow is minimal if there is no subflow with ; equivalently, is minimal if the orbit of every point is dense in . A straightforward application of Zorn’s lemma shows that every -flow has a minimal subflow. This demonstrates that minimal flows exist, but in general it is very difficult to say much about their structure and behavior.
Let be a nonempty compact space. The space of all functions , equipped with the product topology, is also compact, and it becomes a -flow under the action given by
[TABLE]
The -flows of the form are called Bernoulli shifts, or simply shifts. A particularly important case is when is a finite set with the discrete topology; for concreteness, we may then assume that for some . (Here we identify each with the -element set .)
The following notions were introduced by Furstenberg in [Fur67]. Let and be -flows. We view the product space as a -flow equipped with the diagonal action of . A joining of and is a subflow that projects onto and . The -flows and are disjoint, in symbols , if they have only one joining, namely itself. It is not hard to see that if , then at least one of and is minimal.
Recently, Glasner, Tsankov, Weiss, and Zucker obtained the following result:
Theorem 1.1 (Glasner–Tsankov–Weiss–Zucker [Gla+19]).
If is a minimal -flow, then .
For , Theorem 1.1 was proven earlier by Furstenberg [Fur67].
The first step in the proof of Theorem 1.1 in [Gla+19] is a reduction to a combinatorial question concerning the so-called separated covering property of minimal -flows. Somewhat surprisingly, to answer this question, [Gla+19] makes heavy use of group theory; in particular, two classes of groups (namely maximally almost periodic and ICC groups) are treated separately and with completely different arguments. The proof in the ICC case relies on the recent breakthrough results of Frisch, Tamuz, and Vahidi Ferdowsi [FTV19].
In this note, we give a short and self-contained proof of Theorem 1.1 that is purely combinatorial and treats all groups simultaneously. We deduce Theorem 1.1 from the following fact, which is interesting in its own right. Let be a -flow. We say that a set traps a point (or that is trapped in ) if the orbit of is contained in .
Theorem 1.2.
Let and let be a nonempty open set. Then there exists such that for all finite of size at least , the set traps a point.
Theorem 1.1 is derived from Theorem 1.2 in §2. To establish Theorem 1.2, we rely on the so-called Lovász Local Lemma (the LLL for short), an important tool in probabilistic combinatorics introduced by Erdős and Lovász in [EL75]. We state the LLL, in the form we will need, in §3 and use it to prove Theorem 1.2 in §4. While the LLL has been widely used in combinatorics and graph theory for over forty years now, it has only recently become apparent that the LLL can be applied to the study of dynamical systems as well. Several applications of the LLL in ergodic theory and topological dynamics can be found in [ABT19, Ber19, Ber19a, Ber20]; this paper contributes yet another one.
2. Derivation of Theorem 1.1 from Theorem 1.2
Let be a minimal -flow and let be a joining. Our goal is to show that . To this end, let and be nonempty open sets. We have to argue that .
Lemma 2.1.
If is a minimal -flow and is a nonempty open set, then there exists an infinite subset with .
Proof*.*
Since is minimal, the orbit of each point in intersects , and thus . The compactness of implies that there is a finite subset such that . Say that a set is right -separated if for every pair of distinct , . Since is finite while is infinite, there is an infinite right -separated subset . Consider any . For each , we have , i.e., . In other words, for each , there is with . Since is right -separated, the set is infinite, and we are done. ∎
Let be an infinite set as in Lemma 2.1 applied to , and let be the quantity given by Theorem 1.2 applied to . Pick an arbitrary finite subset of size at least and let
[TABLE]
By the choice of , the set traps a point, say . Since projects onto , there is some with . As is minimal and is nonempty open, there is with . Since is trapped in , we have , which means that for some , and since , we also have . Therefore,
[TABLE]
and the proof of Theorem 1.1 is complete.
3. The Lovász Local Lemma
We shall only require a somewhat specialized but simplified version of the Lovász Local Lemma; for a more general discussion of the LLL, the reader is referred to [AS00] and [MR02]. The presentation below follows, with slight modifications, [Ber19a, §1.2].
Let be an arbitrary set and let . A bad (-)event over is a nonempty set of partial functions with finite domains such that for all , , . If a bad event is nonempty, then its domain is the set for any (hence all) ; the domain of the empty bad event is, by definition, the empty set. The probability of a bad -event with domain is defined to be . A map avoids a bad event if there is no such that . Notice that if is finite and is drawn uniformly at random from , then is precisely the probability that does not avoid .
A (/̄)**instance **(of the LLL) over a set is an arbitrary set of bad -events over . A solution to a -instance is a function that avoids every . For an instance and , the neighborhood of in is the set
[TABLE]
The degree of in is defined to be . Let
[TABLE]
An instance is correct for the LLL, or simply correct, if
[TABLE]
where denotes the base of the natural logarithm.
Theorem 3.1 (Erdős–Lovász [EL75]; Lovász Local Lemma).
Let and let be a -instance of the LLL over a set . If is correct for the LLL, then has a solution.
The LLL was introduced by Erdős and Lovász (with in place of ) in their seminal paper [EL75]; the constant was subsequently improved by Lovász (the sharpened version first appeared in [Spe77]).
We should mention that there are two respects in which Theorem 3.1 in the above form is less general then the “full” LLL. First, Theorem 3.1 only works with product probability spaces such as ; this is a special case of the LLL in the so-called variable framework (the name is due to Kolipaka and Szegedy [KS11]). However, although this case is special, it does encompass most typical applications. For the statement of the LLL for general probability spaces, see [AS00, Corollary 5.1.2]. Deducing Theorem 3.1 from [AS00, Corollary 5.1.2] is routine when is finite (see, e.g., [MR02, 41]); the case of infinite then follows by compactness.
Second, there is a more general form of the LLL (often referred to as the General Lovász Local Lemma), that applies to instances without a uniform upper bound on ; see [AS00, Theorem 5.1.1]. However, this more general statement is somewhat technical and we will not need it here.
4. Proof of Theorem 1.2
Let be a finite set. We say that a set is left -separated if for every pair of distinct , .
Lemma 4.1.
If , are finite sets, then has a left -separated subset with
[TABLE]
Proof*.*
First recall some basic facts about finite graphs. Let be a finite graph with vertex set and edge set . A subset is **independent **(in ) if no two vertices in are adjacent to each other. A straightforward greedy construction shows that if every vertex of has at most neighbors, then can be partitioned into independent sets. In particular, has an independent set of size at least .
Now let be the graph with vertex set in which distinct vertices , are adjacent if and only if , or, equivalently, . Every has at most neighbors in (we are subtracting to account for the fact that is not adjacent to itself). Therefore, has an independent set of size at least , and that is precisely what we need. ∎
For a partial map with finite domain, let denote the clopen set given by
[TABLE]
Since the topology on is generated by the sets of the form , it is enough to prove Theorem 1.2 with . So, let be a nonempty finite set and let . Let be such that
[TABLE]
(Such exists since the left-hand side of (4.2) approaches [math] as goes to infinity.) We shall argue that is as desired.
Take any finite set of size at least and let be a set of size at least such that is left -separated (such exists due to Lemma 4.1 applied with in place of ). Define a -instance over as follows. For each , let be the bad -event with domain consisting of all maps such that:
[TABLE]
Notice that since is left -separated, is equal to the disjoint union of the sets , . Let . We claim that if is a solution to , then is trapped in (and hence also in ). Indeed, consider any . Since avoids , the following holds:
[TABLE]
But this precisely means that for some , , i.e., . In view of Theorem 3.1, it only remains to show that is correct for the LLL.
First we bound . Consider any . We need to find an upper bound on the size of the set
[TABLE]
To this end, notice that if and only if . Thus,
[TABLE]
and hence we conclude that . Next we bound . Again, fix and draw uniformly at random. Then for each ,
[TABLE]
and since the sets , are disjoint, we conclude that
[TABLE]
Therefore, . To put everything together, is correct as long as
[TABLE]
Since , (4.2) gives the desired result.
Acknowledgments
I am grateful to Todor Tsankov and Andy Zucker for insightful discussions and to Dima Sinapova for providing stimulating and productive environment during the Logic Fest in the Windy City conference on May 30–June 2, 2019 at the University of Illinois at Chicago. I am also grateful to the anonymous referee for helpful comments.
The reference list from the paper itself. Each links out to its DOI / PubMed record.
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- 4[Ber 19a] A. Bernshteyn “Measurable versions of the Lovász Local Lemma and measurable graph colorings” In Adv. Math. 353 , 2019, pp. 153–223
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