Non-noise sensitivity for word hyperbolic groups
Abstract.
We show that non-elementary random walks on word hyperbolic groups with finite first moment are not noise sensitive in a strong sense for small noise parameters.
1. Introduction
Let be a countable group, and be a probability measure on it. The main interest is in the case when is finitely generated with a finite set of generators and is the uniform distribution on , but we will also consider the case when has an unbounded support. The -random walk starting from the identity is defined by a product of independent sequence of increments with the identical distribution . The noise sensitivity question concerning a -random walk on asks the following: If we choose some real parameter and replace each increment by an independent sample with the same law with probability or retain it with probability , independently, then is the resulting random walk asymptotically independent of the original one?
More precisely, the -random walk starting from is defined by for an independent sequence with the identical distribution and . Let denote the distribution of , which is the -fold convolutions of . For each , let us consider the -random walk on defined by
where denotes the product measure and if and otherwise. For any two probability measures and on a countable set , the total-variation distance is defined by
Definition 1.1.
The -random walk on is called -noise sensitive if for all ,
The -noise sensitivity was introduced by Benjamini and Brieussel [BB21, Definition 2.1]. There it has been shown that this notion in general highly depends not only on but also on . Among others, they have proved that if admits a surjective homomorphism onto the infinite cyclic group and the support of is a finite set of generators, then a -random walk on is not -nose sensitive. Moreover, if is non-Liouville, i.e., there exists a non-constant bounded -harmonic function on , then a -random walk on is not -noise sensitive [BB21, Theorem 1.1]. It is believed that these two properties are the only possible obstructions for the -noise sensitivity for random walks on groups. We show that non-elementary word hyperbolic groups with large class of reveal a strong negation of the -noise sensitivity if is small enough. This also offers in the non-Liouville setting a way to show that random walks are not -noise sensitive in some refined sense for a class of groups possibly without non-trivial homomorphisms onto .
Let be a word hyperbolic group. A probability measure on is called non-elementary if the support generates a non-elementary subgroup as a group. In this setting, it is equivalent to say that contains a free group of rank greater than one (and is necessarily non-elementary). Furthermore we say that has finite first moment if
for some (equivalently, every) word norm . First we note that all -random walk on for a non-elementary is not -noise sensitive without any moment condition.
Theorem 1.2.
Let be a word hyperbolic group and be a non-elementary probability measure on . For all , we have
This in fact follows from the proof of [BB21, Theorem 4.1] due to the non-Liouville property. We provide a proof in this setting to illustrate our approach. Second we show that under the finite first moment condition if is close enough to , then the distribution of a -random walk and the joint distribution of independent copies of two -random walks are mutually singular at infinity.
Theorem 1.3.
Let be a word hyperbolic group and be a non-elementary probability measure with finite first moment on . There exists some such that for all , we have
In the case when is not a non-elementary probability measure, these statements are no longer true. Indeed, it suffices to consider elementary word hyperbolic groups, which are either finite groups or contain as a finite index subgroup (see e.g., [Gro87] and [GdlH90] for background). If is a finite group, then for every probability measure on it, a -random walk on is -noise sensitive. Indeed, and have the same support on and the distributions of corresponding random walks with the same initial state tend to a common stationary distribution for time with the same parity (cf. [BB21, Proposition 5.1]). Benjamini and Brieussel have shown that on the infinite dihedral group, a lazy simple random walk on a Cayley graph is -noise sensitive [BB21, Theorem 1.4].
As it is mentioned above, if has a surjective homomorphism onto , then a -random walk can not be -noise sensitive. This follows by computing covariance of the random walk on each factor of as the image of product of homomorphisms and the classical central limit theorem. The method thus works for with finite second moment. We note, however, that so far this and the non-Liouville property have been the only known ways to disprove -noise sensitivity. See [BB21] and [Kal18, Section 3.3.4] for discussions concerning the subject of matters, various interesting notions of noise sensitivity for random walks on groups, questions and conjectures.
The proofs of Theorems 1.2 and 1.3 rely on the boundary of word hyperbolic groups, in particular, the fact that a -boundary or the Poisson boundary for is realized on a topological boundary of the group. In this setting, we show that if for , then
(1.1) |
where is the asymptotic entropy for a -random walk (see Section 2 for the definition, and Remark 5.1). It is proven by showing that the harmonic measure on the product of boundaries is exact dimensional with a natural (quasi-) metric, i.e.,
where stands for the drift defined by a product metric in (see Theorem 3.1 for the precise statement). The proof follows the methods in [Tan19], adapting to a product of word hyperbolic groups. By (1.1), together with the continuity of in (Corollary 4.2), as it is established by a general result of Erschler and Kaimanovich [EK13], we show that there exists some with for all , deducing Theorem 1.3.
It would be interesting to determine in Theorem 1.3. For example, in the case when is a uniform distribution on a finite set of size , freely generating a free semi-group, the asymptotic entropy is explicitly computed as
and if . This implies that in the special case. It might be expected that in many cases, however, we do not know how to show this in general.
Organization of this paper is the following: In Section 2 we review known facts and tools on random walks and word hyperbolic groups, in Section 3 we show that the harmonic measure for whose marginals are a common non-elementary probability measure on with finite first moment is exact dimensional in Theorem 3.1, in Section 4 the continuity of asymptotic entropy in the parameter is established in Corollary 4.2, following [EK13], in Section 5 we show Theorems 1.2 and 1.3, and in Appendix A, we give a review concerning Poisson boundary for random walks and a proof on continuity of asymptotic entropy for the sake of convenience, mainly for an expository purpose.
Notations
For a real valued function on the set of non-negative integers, we write if as and if there exists a constant such that for all large enough . For a set , we denote by the cardinality, and by its complement set. The set of non-negative integers is written as . We define .
2. Preliminary
2.1. Random walks on word hyperbolic groups and their products
For a countable group and a probability measure on it, the asymptotic entropy of a -random walk is defined by
where , the Shannon entropy for probability measures on , the limit exists by sub-additivity of and is finite if .
Let be a word hyperbolic group. For a probability measure on , let denote the support and we assume that the group generated by as a group is a non-elementary subgroup. We fix a left-invariant word metric associated with some finite set of generators closed under inversion . The following discussion does not depend on the choice of . We denote the associated distance function from the identity by . If has finite first moment, then (cf. [Der86, Section VII, B]).
Let us consider any probability measure on such that the push-forward of on each factor is a fixed on . Let be the probability measure space, where , is the -field generated by the cylinder sets and is the distribution of the -random walk starting from the identity on . The expectation relative to is denoted by . Let be the distribution of . Note that for , each gives the -random walk on starting from for . In this setting, we have for all ,
and the asymptotic entropy of a -random walk is finite since , and is positive since and is a non-elementary subgroup in . We define the metric
Suppose that has finite first moment. Then has finite first moment relative to the distance function . The drift is defined by the limit
where the limit exists by sub-additivity and is finite. The value coincides with the drift of a -random walk relative to , i.e.,
(2.1) |
and also in by the Kingman subadditive ergodic theorem, and since is non-elementary [Kai00, Section 7.3].
2.2. Word hyperbolic groups
We refer to [Gro87] and [GdlH90] for background. Let denote the (Gromov) boundary and we endow with the natural topology which is compact and metrizable. Letting be the Gromov product for based at , we define the quasi-metric in by
Note that satisfies that if and only if , for and the triangle inequality holds up to a multiplicative constant independent of the points. It is known that is bi-Hölder equivalent to a genuine metric in yielding the original topology. We work with the quasi-metric to define balls: Let
For any positive real and , the shadow is defined by
By the hyperbolicity of geodesic metric space , for each fixed , there exist constants , such that for all , all and all in a -neighborhood of a geodesic ray from to , we have
(2.2) |
In the product space , we define
By the definition, the ball of radius centered at in relative to is obtained by
(2.3) |
3. The dimension of harmonic measure
The -random walk on a word hyperbolic group converges to a point in almost surely as in if is non-elementary [Kai00, Theorem 7.6]. This implies that the -random walk on converges to a point in almost surely as in the product space , where and each tends to almost surely for . Let and denote the limiting distribution of on and that of on , respectively. We call and harmonic measures on and on , respectively. Note that the push-forward of on each factor coincides with . The harmonic measure (resp. ) is -stationary (resp. -stationary), i.e.,
(3.1) |
where and , and similarly,
(3.2) |
The and are unique such measures satisfying (3.1) and (3.2), respectively [Kai00, cf. Theorem 2.4]. Concerning more on background, see [Kai00].
For the harmonic measure for the -random walk, we show the following:
Theorem 3.1.
Let be a word hyperbolic group and be a non-elementary probability measure on with finite first moment. If is a probability measure on such that the push-forward of on each factor is , then the corresponding harmonic measure on is exact dimensional, i.e.,
where is the asymptotic entropy, is the drift relative to for the -random walk on and the ball is defined by in .
Let us define the (upper) Hausdorff dimension of by
where stands for the Hausdorff dimension of relative to in . Theorem 3.1 together with the Frostman-type lemma (cf. [Tan19, Section 2.2]) shows the following:
Corollary 3.2.
In the setting of Theorem 3.1, we have
Let us keep the same setting and notations as in Theorem 3.1 throughout this section. We use the following ray approximation of a -random walk on a word hyperbolic group : Let be a Borel measurable map from to the space of unit speed geodesic rays from in endowed with the topology of convergence on compact sets. (Here is defined as a Borel measurable map by choosing a total order on a fixed set of generators and the lexicographical minimal geodesic for each point in the boundary.) Letting
we have
(3.3) |
[Kai00, Section 7.4], where one should write instead (the integer part of ) here and below, however, we keep “” for the sake of simplicity. Let us define the map
as a Borel measurable map. For a -random walk on , we have by (3.3),
(3.4) |
Recall that the Shannon theorem for random walks:
(3.5) |
which follows from the Kingman subadditive ergodic theorem ([KV83, Theorem 2.1] and [Der80, Section IV] where Y. Derriennic attributes to an observation by J. P. Conze).
First we show the dimension upper bound in the claim.
Lemma 3.3.
For -almost all in ,
Proof.
For all and all interval in , let
Since has finite first moment, for for all large for -almost every in , and by (2.1) and (3.5), there exists an such that . Let . For each , let
which defines the event where a -random walk after time is . The conditional probabilities satisfy that
(3.6) |
Indeed, letting and for simplicity of notation, we have for , and by the Markov property of the -random walk,
Let denote the -algebra generated by . Since for -almost every ,
we have by the bounded martingale convergence theorem,
as , where . Furthermore, since for -almost every ,
we have
as . Note that for -almost every . Indeed, letting , we have almost everywhere in , whence integrating both sides yields . Thus we obtain (3.6).
For -almost every , we have for each ,
whence is defined and
for a constant independent of or (cf. [Kai00, Section 7.2]). For -almost every , since , by the -hyperbolicity we have
and thus we obtain by (2.3), for -almost every ,
where is a positive constant depending only on the metric of the group . Therefore for -almost every ,
Moreover, by the definition of , we have for all . Invoking (3.6), we obtain
Noting that satisfy that for all , we have
Since and for all , we obtain
as required. ∎
Next we show the dimension lower bound. We use the following lemma.
Lemma 3.4.
For every there exists a Borel set in such that and
Proof.
Let be the conditional probability measures associated with , where we have
For all and all positive integer , if we define
then by (3.4) and (3.5), there exists an such that . Letting , we define
Since
we have .
Let be any sequence with for . Note that for -almost every and for all , if , then
for a positive constant depending only on the hyperbolicity constant of the metric in , and thus
where for and for a fixed . This shows that for all ,
The second term is estimated as follows:
Therefore we obtain
(3.7) |
for all . Moreover, since
we have for all ,
(3.8) |
where is a constant greater than the exponential growth rate of , i.e.,
Combining (3.7) and (3.8), we obtain
Let us define for -almost every for all . By (2.2) and (2.3), as in a similar way in the last part in the proof of Lemma 3.3, for -almost every ,
for a constant . Since for all , we have
Replacing by a small enough constant yields the claim as stated. ∎
Lemma 3.5.
For -almost all in ,
Proof.
For all , let be the Borel set in Lemma 3.4. For the hyperbolic metric space and the boundary , we have that for each , the space admits a bi-Lipschitz embedding into the Euclidean space for some [BS00, Theorem 9.2]. Hence there exists a bi-Lipschitz map ,
i.e., for a constant ,
for all , , where denotes the standard Euclidean norm in . By the Lebesgue density theorem for the Borel measure in , we have
where stands for the standard Euclidean (closed) ball in . This implies that
and for -almost all , there exist positive constants and such that
Therefore we obtain
Lemma 3.4 implies that
and since and for all ,
concluding the claim. ∎
4. Continuity of entropy
For a countable group (in particular we discuss a product of word hyperbolic groups), we endow the set of probability measures on with the topology induced by the total variation distance. Note that for all probability measure and all sequence of probability measures we have
if and only if as for each . Fix a left-invariant metric on with finite exponential growth rate and let for . For a finite set in , let
Erschler and Kaimanovich have shown that the continuity of in under some general conditions [EK13]. We say that a set of probability measures on satisfies uniform first moment condition if
(M) |
for all sequence of finite sets with . We assume that there exists a pair of Borel -spaces , such that the -space with the diagonal action admits a -invariant Borel set in and a -equivariant map assigning to a proper subset (strip) in . Let us say that the strips given by the map satisfy uniform subexponential growth if
(G) |
For non-negative real , letting be the -neighborhood of , we define
Note that the union of over covers . If a pair of Borel -spaces and admits a probability measure on (resp. on ) for which (resp. ) is a - (resp. -) boundary (where for ), and further
(S) |
then we say that satisfies uniform strip condition.
Theorem 4.1 (Theorem 1 in [EK13]).
Theorem 4.1 applies to word hyperbolic groups and their products with sequences of probability measures: In the case when is a word hyperbolic group, for a sequence of probability measures on with uniform first moment converging to a probability measure , we have as [EK13, Theorem 2]. Actually, it suffices to consider the case when is a non-elementary word hyperbolic group and the limiting probability measure is non-elementary. One may take the Gromov boundary endowed with the harmonic measures and , respectively, and , which is open in the product . Furthermore, for the strip is defined as the union of bi-infinite geodesics connecting and in a Cayley graph of . The condition (G) is satisfied since
where the implied constant depends only on the Cayley graph. Furthermore the condition (S) is satisfied. Indeed, the harmonic measure is the unique -stationary measure on and the measures weakly converge to as , and is supported on an open set . Letting denote the interior of , we have
for every subsequence of . Noting that increases and exhausts as grows, we have (S) (cf. [EK13, Lemma 3]).
In the case when the group is a product of word hyperbolic groups and a probability measure , one may take and
where and , and is open in . The strip is defined by
and we have
This shows that (G) holds. Moreover we have (S) for a sequence of probability measures on since is the unique -stationary measure on and supported on an open set as in the case on presented above.
Corollary 4.2.
For a word hyperbolic group and a non-elementary probability measure with finite first moment, the asymptotic entropy is continuous in .
5. Proofs of Theorems 1.2 and 1.3
Proof of Theorem 1.2.
For probability measures and on , the total variation distance is defined by
For each , a -random walk converges to in as in , -almost surely, and the distribution converges weakly to the harmonic measure (see the beginning of Section 3). Therefore for , we have
(5.1) |
For all , we have . Indeed, suppose that for some , then we have
since is the -stationary measure on (cf. (3.1) and (3.2) in Section 3). Noting that is the -stationary measure on , we have
and
This shows that is the -stationary (harmonic) measure by the uniqueness. However, the harmonic measure for is supported on the diagonal in and is non-atomic on since is non-elementary, we have , yielding a contradiction. Therefore for all , we have , and thus by (5.1),
as claimed. ∎
Proof of Theorem 1.3.
As in the same way in the beginning of the proof of Theorem 1.2, for all , we have
Theorem 3.1 shows that for the Borel set
we have . By Corollary 4.2, the function for is continuous. Furthermore,
and since is non-elementary. Hence there exists such that for all . This shows that for all , we have and , implying that and are mutually singular and . Therefore we have for all ,
and , as required. ∎
Remark 5.1.
Appendix A A proof of Theorem 4.1
In this section, denotes the expectation for a probability measure . Let be a countable group endowed with a probability measure of finite entropy, i.e., . For the -random walk starting from on , let us consider the probability measure space , where is the -field generated by the cylinder sets and is the distribution of .
For each positive integer , let be the measurable partition on where and belong to the same set if and only if for all . For any sub -field in , the conditional entropy is defined by
where stands for the conditional probability measure with respect to . The tail -field is defined by . In the case when , letting , we have
(A.1) |
[KV83, cf. Proof of Theorem 1.1].
The group acts on by for . The stationary -field is the sub -field of generated by shift-invariant measurable sets, where the shift is defined by on . Note that is -invariant, i.e., if , then for all . By definition, we have , and it is known that their -completions coincide, i.e., mod [KV83, Section 7.0] (where it is crucial that the initial state is a point). Therefore by (A.1),
(A.2) |
For each -invariant sub -field of , let for -almost every , and let
and we define the entropy of conditional process: For , let
(A.3) |
This yields , and in particular, in the case when , by (A.2), we obtain for all ,
(A.4) |
[Kai00, Sections 3 and 4].
We write for simplicity of notations.
Lemma A.1.
For a set of probability measures on with uniform first moment condition, the function ,
is continuous.
Proof.
For the exponential growth rate for , let us fix and define
For the ball in with large enough, decomposing the sum
we estimate the second and third terms. First, we have
Second, letting for non-negative integers ,
for constants and , for all large enough , where in the first inequality we have used for and large enough. Finally, we obtain
This shows that
implying that is continuous on . ∎
Lemma A.2.
In the same setting as in Lemma A.1, for all and for all positive integer ,
(A.5) |
and
(A.6) |
where , and are positive constants independent of and . Moreover, for each , the function , is continuous.
Proof.
We use the same notation as in the proof of Lemma A.1 and obtain (A.6) in the same way for each positive integer and for all . Let us show (A.5). Note that
where the last equality follows since are independent and identically distributed. Moreover, we have
where the first term is at most
and the second term is at most
by the Markov inequality. Therefore for all and for all , we have and
yielding (A.5). Finally, since for , , the term
is continuous in for each fixed , and converges to uniformly on in as by (A.6), the last statement holds. ∎
Recall the notations from [Kai00, Section 6]: Let be the probability measure space of bilateral paths with . The space is identified with the product space via the map from to where and is the distribution of -random walk starting from . We denote by the probability measure preserving transformation on induced from the Bernoulli shift in the space of increments, more explicitly,
Given -equivariant measurable maps and for the -boundary and for the -boundary , let us define by and by . Note that and .
Proof of Theorem 4.1.
The condition (S) implies that
where for , and thus
uniformly on . Moreover, since the map is -equivariant and is -invariant, we have
Therefore, disintegrating the measure,
we obtain
(A.7) |
By Lemma A.2 (A.5), for all and for all ,
and thus letting
we have as by the condition (M), and by the Markov inequality,
and as . Hence for all and all , we have , and this yields by disintegration,
(A.8) |
For all , let us take any and satisfying that and . Noting that
(A.9) |
Furthermore, the condition (G) implies that for all and all , there exists a sequence of positive reals such that
(A.10) |
and as .
Let us estimate the conditional entropy in (A.3). For the simplicity of notations, let
First we have by the Jensen inequality and by (A.10),
and thus,
(A.11) |
where we have used for .
Second by (A), we have , and thus by the Jensen inequality,
and as in a similar way to (A.11),
(A.12) |
for and all large enough . By (A.11) and (A), noting that , we have
(A.13) |
for all large enough .
Acknowledgment
The author would like to thank Jérémie Brieussel for bringing him the problem and discussions, and an anonymous referee for beneficial comments. This work is partially supported by JSPS Grant-in-Aid for Scientific Research JP20K03602.
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