Let P be a finite nonempty set of primes, and let SP be the multiplicative semigroup that they generate. We prove that there are an invertible weakly mixing measure-preserving transformation T and a set A of positive measure such that A∩T−rA=∅ for every r∈SP. This gives a negative answer to Bergelson's 1996 question concerning recurrence along {2m3n:m,n≥1}, and applies to every finitely generated multiplicative semigroup of positive integers. More generally, we give a sufficient condition for weakly mixing non-recurrence based on divisibility properties and separation by finitely many rotations of the circle. This criterion also applies to an infinitely generated multiplicative semigroup not contained in any SP with P finite.
Introduction
Poincaré’s recurrence theorem guarantees that a set of positive measure in a measure-preserving system returns to itself. One may ask whether the return time can be required to belong to a prescribed set of integers. Write N={1,2,…} and N0={0,1,2,…}. A set R⊂N is a set of measurable recurrence if, for every invertible measure-preserving system (X,B,μ,T) and every A∈B with μ(A)>0, there is an r∈R such that μ(A∩T−rA)>0.
Consider the multiplicative semigroup R2,3={2m3n:m,n≥1}. Since none of its elements is divisible by 5, rotation by 1 on Z/5Z shows that R2,3 is not a set of measurable recurrence. However, weakly mixing systems have no nontrivial measurable rotation factors, so this example does not answer the question for weakly mixing systems. In 1996, Bergelson [3 Question 3] asked whether every invertible weakly mixing system and every set A of positive measure satisfy
μ(A∩T−2m3nA)>0for some m,n≥1.
Frantzikinakis, Host, and Kra recorded this question as open in their 2025 paper [7 Section 3.2].1 By modifying a construction of Maucourant [10 Lemma 4.2], they showed that R2,3 can fail to be recurrent even for a totally ergodic torus rotation. They also proved that the larger set {k!2m3n:k,m,n≥1} is Bohr recurrent, that is, recurrent for every finite-dimensional torus rotation [7 Theorem 1]. We give a negative answer to Bergelson’s question. The result holds for multiplicative semigroups generated by any finite nonempty set of primes.
Theorem 1.1. Let P={p1,…,pd} be a finite nonempty set of primes and put
SP={p1n1⋯pdnd:n1,…,nd∈N0}.
There exist a standard nonatomic probability space (X,B,μ), an invertible weakly mixing probability-preserving transformation T:X→X, and a Borel set A⊂X such that μ(A)>0 and A∩T−rA=∅ for every r∈SP.
The system can be chosen to be a finite product of two-sided complex Gaussian shifts.
Every finitely generated multiplicative semigroup of positive integers is contained in some SP, since only finitely many primes divide its generators. Thus the theorem applies to all such semigroups, including the time 1. Taking P={2,3} answers Bergelson’s question. Coding the set A also gives a compact topologically weakly mixing subshift with a nonempty clopen set having no return at any time in SP; see Proposition 4.7.
Our argument also applies to sets involving infinitely many distinct primes. Write T=R/Z and e(t)=exp(2πit). A set R⊂N is Bohr recurrent if, for every m≥1, α1,…,αm∈T, and ε>0, there exists r∈R such that max1≤a≤m∣e(rαa)−1∣<ε. For a nonempty set H⊂N, gcdH denotes the greatest positive integer dividing every member of H. We first prove the following general theorem.
Theorem 1.2. Let R⊂N be of the form
R=F∪E1∪⋯∪Ed,
where d≥1, F is finite, and E1,…,Ed are infinite. Suppose that
N→∞limgcd{r∈Ei:r≥N}=∞(1≤i≤d).(1)
Suppose also that there are α1,…,αm∈T, with m≥1, and δ>0 such that
1≤a≤mmax∣e(rαa)−1∣≥δ(r∈R).(2)
Then there exist a standard nonatomic probability space (X,B,μ), an invertible weakly mixing probability-preserving transformation T:X→X, and a Borel set A⊂X such that μ(A)>0, A∩T−rA=∅(r∈R).
The system can be chosen to be a finite product of two-sided complex Gaussian shifts.
Condition (1) says that arbitrarily large integers divide all but finitely many members of each Ei. Condition (2) says that R is not Bohr recurrent; compare the definition in [7 Section 1.1]. The divisibility condition alone does not suffice, as the example in Remark 3.2 shows. For SP, assign each integer to a prime with maximal exponent. The resulting sets satisfy (1), and a prime outside P gives (2). Section 4 also gives an infinitely generated example and proves non-recurrence for (SP+h)∩N for every fixed h∈Z.
The Gaussian construction associates continuous measures on the circle with weakly mixing systems; see [8 Section 2]. Related constructions of perfect sets and continuous measures under divisibility assumptions appear in Eisner and Grivaux [6, Propositions 3.8 and 3.9]. Grivaux’s non-recurrence criterion [8 Theorems 1.1 and 2.6] combines separation by a rotation with uniform approximation: for an infinite set Q⊂N containing 1, one requires unit complex numbers λk=1 such that supr∈Q∣λkr−1∣→0. For a single prime, weakly mixing non-recurrence, including the corresponding result for integer translates, follows from [8 Theorem 1.2]. For multiplicative semigroups, Badea and Grivaux [2 Section 6.1] group the elements according to a maximal prime exponent and construct continuous measures whose Fourier coefficients tend to 1 within each group. This convergence alone does not ensure that
r∈Q∑∫T∣e(rt)−1∣2dν(t)
is small enough for the Gaussian argument. It also does not give the uniform approximation required by Grivaux’s criterion.
Our proof starts with a finite partition of SP. Following Badea and Grivaux [2 Section 6.1], we assign each element to a prime with maximal exponent in its factorization. In each part, the exponent of the chosen prime tends to infinity as the elements tend to infinity. Thus every power of that prime divides all sufficiently large elements of the part.
Fix η>0, to be chosen sufficiently small below, and one part E. Choose denominators Dj and integers 1=N0<N1<N2<⋯ in the order D1,N1,D2,N2,…, so that Dj divides every r∈E with r≥Nj. For ϵ=0,1, let Qϵ consist of those r∈E lying in an interval [Nj,Nj+1) with j≡ϵ(mod2). For each Qϵ, consider the random series
Θϵ=ℓ≥1ℓ≡ϵ(mod2)∑Dℓωℓ,ϵ=0,1,
where the digits ωℓ are independent, each equal to 0 or 1 with probability 1/2. We take the sums modulo one. Choose the denominators large enough and make them grow fast enough that, for each ϵ, different choices of the digits used in Θϵ give different points of T. Each such digit sequence has probability zero, so the distribution of each series has no atoms.
Now take r∈Qϵ∩[Nj,Nj+1), so that j≡ϵ(mod2). The denominators of the terms of Θϵ with indices at most j divide r. After multiplication by r, these terms are integers. They therefore do not change the value of e(rΘϵ), which depends only on the remaining terms. Since j+1 has the opposite parity, the remaining terms have indices j+2,j+4,….
When we choose Dj+2, the endpoint Nj+1 is already fixed, and every r in the interval satisfies r<Nj+1. We can therefore choose Dj+2 and the later denominators large enough to make ∣e(rΘϵ)−1∣ as small as needed, uniformly for all r∈Qϵ∩[Nj,Nj+1) and all choices of the digits. Since there are finitely many such r, we can also make the sum of the squared bounds over the interval as small as needed. We choose the bounds for these interval sums so that their total is less than η. Since the bounds do not depend on the digits, the same estimates hold on the supports of the measures. Grivaux [8 Fact 4.2 and Section 4] also uses alternating finite intervals to obtain summable errors. Here we choose each denominator to divide all sufficiently large elements of the corresponding part.
Thus, for every η>0, we obtain a finite partition of SP and, for each part Q, a continuous probability measure ν on T such that
r∈Q∑t∈suppνsup∣e(rt)−1∣2<η.
The partition and measures may depend on η.
We now use this estimate to build a weakly mixing system with no returns along Q. Take a prime q∈/P and put ζ=e(1/q). No element of SP is divisible by q. Hence there is a constant δ>0 such that ∣ζr−1∣≥δ for all r∈SP. Translate ν by 1/q to obtain a continuous probability measure σ. Let (X,μ,T) be the complex Gaussian shift associated with σ, with coordinates Zk=Z0∘Tk. The shift is invertible and weakly mixing. Its coordinates satisfy
E∣Zr−ζrZ0∣2=∫T∣e(rt)−1∣2dν(t).
Thus the sum of these mean square errors over r∈Q is less than η.
Set a=δ/8 and let C={∣Z0−1∣<a}. Since Z0 is standard complex Gaussian, μ(C)>0 depends only on a, not on ν. On C∩T−rC, we have ∣Z0−1∣<a,∣Zr−1∣<a. Together with ∣ζr−1∣≥δ, this gives ∣Zr−ζrZ0∣>δ−2a>δ/2. By Markov's inequality,
r∈Q∑μ(C∩T−rC)≤δ24r∈Q∑E∣Zr−ζrZ0∣2<δ24η.
Since μ(C) depends only on a, we apply the preceding construction with η small enough that 4η/δ2<μ(C)/2.
Remove from C all points that return to C at a time in Q, and set A=C∖⋃r∈QT−rC. The sum bound gives μ(A)>μ(C)/2>0. Also, A⊂C and A∩T−rC=∅ for every r∈Q. Therefore A∩T−rA=∅ for all r∈Q. The bound on the sum is needed because we remove the return events for all r∈Q.
Apply this construction to each part of the partition. Take the product of the systems and the product of the sets. The finite product is weakly mixing, and the product set has positive measure. Every r∈SP belongs to one part. The set in that coordinate has no return at time r, so neither does the product set.
The arithmetic construction only uses arbitrarily large integers that divide all sufficiently large elements of each part. It therefore applies beyond finitely generated multiplicative semigroups. If finitely many rotations give a uniform separation from 1, we further partition each part so that one rotation gives this separation on each new part. The same Gaussian construction and finite product argument then prove Theorem 1.2. The choice of denominators also gives the uniform approximation used in Corollary 4.5 to prove fixed integer translates via Grivaux’s criterion.
Organization of the paper. Section 2 recalls the necessary preliminaries and establishes a Gaussian criterion for non-recurrence. Section 3 constructs continuous measures with summable Fourier errors and proves the general theorem. Section 4 applies this result to multiplicative semigroups, integer translates, and symbolic systems.
Preliminaries and Gaussian non-recurrence
Probability measures and weak mixing
A probability space (X,B,μ) consists of a set X, a σ-algebra B, and a countably additive measure with μ(X)=1. We work with standard Borel spaces: these are measurable spaces isomorphic to a complete separable metric space with its Borel σ-algebra. A measure has no atoms if every measurable set of positive measure contains a measurable subset of strictly smaller positive measure. On a standard Borel space this is equivalent to every singleton having measure zero. A Borel measure on T is called continuous when it has no atoms.
For a measurable map f:X→Y, its pushforward is (f∗μ)(B)=μ(f−1(B)). For every nonnegative measurable function h, and every integrable h,
∫Yhd(f∗μ)=∫Xh∘fdμ.
For a Borel probability measure on a separable metric space, its support is
suppμ={x:μ(V)>0 for every open neighbourhood V of x}.
It is closed and has full measure: its complement is a countable union of measure-zero basic open sets. The measure has full support on X if every nonempty open subset of X has positive measure. We write 1A for the indicator of A.
An invertible measure-preserving system (X,B,μ,T) consists of a probability space and a measurable bijection T:X→X with measurable inverse and T∗μ=μ. For r∈Z, we use T−rA={x:Trx∈A}. The transformation is ergodic if μ(T−1A△A)=0 implies μ(A)∈{0,1}, where △ denotes symmetric difference. It is weakly mixing if, for all bounded measurable complex functions f,g,
N1n=1∑N∫f(g∘Tn)dμ−∫fdμ∫gdμ⟶0.(3)
Equivalently, T×T is ergodic for μ×μ; see [5]. Taking indicators gives the equivalent set formulation with μ(A∩T−nB)−μ(A)μ(B).
For a Borel probability measure σ on T, write
σ(n)=∫Te(nt)dσ(t)(n∈Z).
Then σ(0)=1 and σ(−n)=σ(n). For a topological space X, we write B(X) for its Borel σ-algebra. All sequence spaces below carry the product topology, with C carrying its usual topology and {0,1} the discrete topology.
Random variables and Gaussian shifts
Let (Ω,F,ρ) be a probability space. A complex random variable is a measurable map W:Ω→C. For integrable W, write EρW=∫ΩWdρ, omitting the subscript when the measure is clear. The distribution of a random vector W:Ω→Cm is the pushforward measure W∗ρ.
A standard complex Gaussian random variable is a random variable of the form
Z=2X+iY,
where X and Y are independent real random variables with density (2π)−1/2e−t2/2 on R. The density of Z with respect to Lebesgue area measure on C is π−1e−∣z∣2. In particular,
EZ=EZ2=0,E∣Z∣2=1.
The following Gaussian construction is classical; see [9 Appendix C]. We use its complex-valued formulation from [1 Theorem 2.3 and Proposition 2.5].
Lemma 2.1. Let σ be a Borel probability measure on T. There exists a Borel probability measure γσ on CZ such that the coordinate functions Zk(z)=zk, k∈Z, are standard complex Gaussian random variables satisfying
E(ZkZl)=σ(k−l),
E(ZkZl)=0(k,l∈Z).
The measure γσ has no atoms. The shift
T:CZ→CZ,(Tz)k=zk+1,
is invertible and preserves γσ. If σ has no atoms, then (CZ,γσ,T) is weakly mixing.
Proof. Set φ(n)=σ(n), for any n∈Z. Since σ is a probability measure, φ(0)=1. Moreover, for any n1,…,nm∈Z and c1,…,cm∈C,
Thus φ is positive definite, and [1 Theorem 2.3] applies.
That theorem gives a Borel probability measure γσ on CZ, invariant under the shift (Sz)k=zk−1. The coordinate functions Zk(z)=zk satisfy
EZk=0,
E(ZkZl)=φ(k−l)=σ(k−l),(k,l∈Z),
E(ZkZl)=0.
Since these variables are Gaussian and σ(0)=1, each Zk is standard complex Gaussian. Define T=S−1. Then (Tz)k=zk+1. Since S is invertible and preserves γσ, so does T.
Since Z0 is standard complex Gaussian, it has density π−1e−∣w∣2 on C. Thus γσ({Z0=a})=0 for every a∈C. For every z=(zk)k∈Z∈CZ, we have {z}⊂{w∈CZ:Z0(w)=z0} and hence γσ({z})≤γσ({Z0=z0})=0. Therefore γσ has no atoms.
Finally, suppose that σ has no atoms. By [1 Proposition 2.5], the Gaussian system associated with σ, namely (CZ,γσ,S), is weakly mixing. Since weak mixing is preserved under inversion, (CZ,γσ,T) is also weakly mixing. □
We call (CZ,γσ,T) the complex Gaussian shift associated with σ. For later use, note that Z0∘Tn=Zn, so
∫(Z0∘Tn)Z0dγσ=σ(n)(n∈Z).
A Gaussian non-recurrence criterion
The following estimate uses the Gaussian non-recurrence argument of Grivaux [8, Proposition 4.5]; see also [4 Section 4]. It combines separation by a rotation with a summable bound on return events. We formulate the argument for coordinate Gaussian shifts and include explicit constants for later use.
Proposition 2.2. Let Q⊂N be nonempty, and suppose that ζ∈C and δ>0 satisfy
∣ζ∣=1,∣ζr−1∣≥δ(r∈Q).
Set
a=8δ,cδ=a2e−(1+a)2.
Suppose there is a continuous Borel probability measure ν on T such that
r∈Q∑∫T∣e(rt)−1∣2dν(t)<8δ2cδ.
Then there exist an invertible weakly mixing complex Gaussian shift (X,B,μ,T) and a Borel set A⊂X satisfying
μ(A)>2cδ,A∩T−rA=∅(r∈Q).
Proof. Choose α∈T with ζ=e(α). Define a Borel probability measure σ on T by
σ(B)=ν(B−α)
for every Borel set B⊂T. Since ν is continuous, so is σ. Moreover,
σ(r)=∫Te(r(t+α))dν(t)=ζrν(r).
By Lemma 2.1, let
X=CZ,B=B(CZ),μ=γσ,
and define
T:X→X,(Tz)k=zk+1.
Then (X,B,μ,T) is an invertible weakly mixing measure preserving system. For k∈Z, let Zk:X→C be the coordinate function Zk(z)=zk. Each Zk is a standard complex Gaussian random variable. In particular,
Finally, A⊂C and A∩T−rC=∅ for every r∈Q. Since T−rA⊂T−rC, we obtain
A∩T−rA=∅(r∈Q).
Products and finite sets of times
We use the following finite product argument to combine the sets of times; compare [4 Section 4].
Lemma 2.3. Let (Xj,Bj,μj,Tj), 1≤j≤l, be finitely many invertible weakly mixing probability-preserving systems, and let (X,B,μ,T) be their product. Then T is invertible, probability preserving, and weakly mixing. If Qj⊂N and Aj∈Bj satisfy μj(Aj)>0 and Aj∩Tj−rAj=∅ for every r∈Qj, then A=∏j=1lAj satisfies
μ(A)>0,A∩T−rA=∅(r∈j=1⋃lQj).
Proof. The product of finitely many weakly mixing systems is weakly mixing; see [4 Section 4]. Moreover,
Lemma 2.4.For every finite set H⊂N, there are an invertible weakly mixing two-sided complex Gaussian shift (X,B,μ,T) and a Borel set B of positive measure such that B∩T−rB=∅ for all r∈H.
Proof. Take the Gaussian shift in Lemma 2.1, with σ equal to normalized Lebesgue measure on T. Its coordinates are independent standard complex Gaussian variables, and the shift is weakly mixing. Put L=max(H∪{0}) and
B={∣Z0−1∣<1/4}∩k=1⋂L{∣Zk∣<1/4}.
By independence and the positivity of the Gaussian density, μ(B)>0. For every r∈H, if x∈B∩T−rB, then
∣Zr(x)∣<1/4,∣Zr(x)−1∣=∣Z0(Trx)−1∣<1/4.
Hence
1≤∣Zr(x)∣+∣Zr(x)−1∣<1/2,
a contradiction. Thus B∩T−rB=∅ for all r∈H.
Divisibility and spectral measures
We divide the given set of positive integers into two parts and construct a continuous probability measure for each part. For each measure, we bound ∣e(rt)−1∣ uniformly over its support and make the sum of the squared bounds over all integers in the corresponding part as small as needed. We will also use this construction to prove integer translates in Corollary 4.5.
The reciprocal-denominator series below are closely related to the constructions of Eisner and Grivaux [6 Propositions 3.8 and 3.9] and Maucourant [10 Lemma 4.2]. Maucourant uses separate even- and odd-indexed series: divisibility makes the earlier terms integers after multiplication, while the remaining terms are small. Grivaux [8 Fact 4.2] also uses alternating finite intervals to obtain summable estimates. Here we use random digits and choose denominators dividing all sufficiently large elements of the relevant set, so that the resulting estimates are uniform on the supports of the measures.
Lemma 3.1.Let E⊂N be infinite and suppose that
gcd{r∈E:r≥N}⟶∞(N⟶∞).
Then for every η>0, there are a partition E=C0⊔C1 into infinite sets and continuous Borel probability measures ν0,ν1 on T such that, with Qϵ=Cϵ∪{1},
r∈Qϵ∑t∈suppνϵsup∣e(rt)−1∣2<η(ϵ=0,1).
For each of these fixed sets Qϵ, there are unit complex numbers λϵ,k=1 satisfying
λϵ,k⟶1,r∈Qϵsup∣λϵ,kr−1∣⟶0(k⟶∞).(4)
The partition and measures may depend on η.
Proof. For each N, the integer gcd{r∈E:r≥N} divides all but finitely many members of E. Hence the hypothesis implies that
D={D∈N:D divides all but finitely many members of E}
is unbounded. Set D0=N0=1. After Dj−1 and Nj−1 have been fixed, choose Dj∈D so that
Dj≥4Dj−1,Dj≥2jNj−1,Dj216π2Nj−13<η2−j(j≥1),
and then choose an integer Nj>Nj−1 such that
Dj∣r(r∈E,r≥Nj),E∩[Nj−1,Nj)=∅.
Such an Nj exists because Dj∈D and E is unbounded. No divisibility between successive Dj is required. Define
Every interval meets E, so E=C0⊔C1 and both sets are infinite. For ϵ∈{0,1}, let Ωϵ={0,1}Iϵ be equipped with the product probability measure Pϵ under which each coordinate takes the values 0 and 1 with equal probability. For ω=(ωℓ)ℓ∈Iϵ∈Ωϵ, define
Θϵ(ω)=ℓ∈Iϵ∑Dℓωℓ.
We define a probability measure νϵ on T by
νϵ(B)=Pϵ{ω∈Ωϵ:Θϵ(ω)mod1∈B}
for every Borel set B⊂T. Since Dℓ+1≥4Dℓ and D1≥4, we have
0≤Θϵ(ω)≤ℓ=1∑∞Dℓ1≤D11ℓ=0∑∞4−ℓ=3D14≤21.
The series converges uniformly on the compact space Ωϵ. Thus Θϵ is continuous on Ωϵ. Consequently,
Kϵ={ℓ∈Iϵ∑Dℓωℓ(mod1):ωℓ∈{0,1}}
is compact. By the definition of νϵ, νϵ(Kϵ)=1, and suppνϵ⊂Kϵ.
Let ω=ω′, and let ℓ∈Iϵ be the first index at which they differ. Then
Hence, for ω=ω′, 0<∣Θϵ(ω)−Θϵ(ω′)∣≤21<1. In particular, Θϵ(ω)−Θϵ(ω′)∈/Z. Thus Θϵ(ω)≡Θϵ(ω′)(mod1), and then for every t∈Kϵ, there is a unique ω∈Ωϵ such that
Θϵ(ω)=t(mod1).
Finally, we show that νϵ has no atoms. Fix a=(aℓ)ℓ∈Iϵ∈Ωϵ. For every integer M≥1, independence gives
Pϵ({ω=a})≤Pϵ(ω2i−ϵ=a2i−ϵ for 1≤i≤M)=i=1∏MPϵ(ω2i−ϵ=a2i−ϵ)=2−M.
Letting M→∞, we obtain Pϵ({ω=a})=0. Since ω↦Θϵ(ω) (mod 1) is injective, for every t∈T the set
{ω∈Ωϵ:Θϵ(ω)≡t(mod1)}
contains at most one element. Since every singleton in Ωϵ has probability zero, we obtain
νϵ({t})=Pϵ(Θϵ(ω)≡t(mod1))=0.
Hence νϵ is a continuous probability measure.
Fix r∈E∩[Nj,Nj+1), where j≡ϵ(mod2). For every ℓ∈Iϵ with ℓ≤j, we have r≥Nj≥Nℓ. By the choice of Nℓ, Dℓ∣r, Dℓrωℓ∈Z. Since j+1∈/Iϵ, it follows that
Write the nonempty sets among F and Ri,ε,a as Q1,…,QL. Then L≤2dm+1. By Proposition 2.2 and Lemma 2.4, for each Qj there is a weakly mixing Gaussian shift (Xj,μj,Tj) and a Borel set Aj such that
μj(Aj)>0,Aj∩Tj−rAj=∅(r∈Qj).
Now set
(X,μ,T)=j=1∏L(Xj,μj,Tj),A=j=1∏LAj.
By Lemma 2.3, T is weakly mixing, and
μ(A)=j=1∏Lμj(Aj)>0,A∩T−rA=∅(r∈R).
This completes the proof. □
Remark 3.2. Condition (1) alone does not guarantee non-recurrence. Consider
R∗=k>1⋃{j2k:1≤j≤k}.
We first show that R∗ is a set of recurrence. Let (X,B,μ,T) be an invertible probability-preserving system, and let A∈B satisfy μ(A)>0. Choose k≥1 such that (k+1)μ(A)>1. Since
j=0∑kμ(T−j2kA)=(k+1)μ(A)>1,
there exist 0≤i<j≤k such that
μ(T−i2kA∩T−j2kA)>0.
By invariance of μ,
μ(A∩T−(j−i)2kA)>0.
Since (j−i)2k∈R∗, the set R∗ is recurrent; compare [8 Remark 3.1]. On the other hand, for every K≥1, all elements of R∗ outside the finitely many sets
{j2k:1≤j≤k},1≤k<K,
are divisible by 2K. Hence
N→∞limgcd{r∈R∗:r≥N}=∞.
Thus R∗ satisfies the divisibility condition (1) but cannot satisfy (2).
Applications
Finitely generated semigroups
We use the partition according to a maximal exponent from [2 Section 6.1].
Lemma 4.1. Let R⊂N be infinite, let p1,…,pd be distinct primes, with d≥1, and write vpi(r)=max{k∈N0:pik∣r}. Suppose that
#{r∈R:1≤i≤dmaxvpi(r)<K}<∞for every integer K≥1.
Then R=F∪E1∪⋯∪Es, where F is finite, 1≤s≤d, each Ei is infinite, and
gcd{r∈Ei:r≥N}⟶∞(N→∞,1≤i≤s).
Proof. For each r∈R, choose the smallest index i for which vpi(r) is maximal. More precisely, set i(r)=min{i:vpi(r)=max1≤j≤dvpj(r)}, Gi={r∈R:i(r)=i}. Then
R=i=1⋃dGi.
Fix 1≤i≤d. We show that if Gi is infinite, then
N→∞limgcd{r∈Gi:r≥N}=∞.
Let K≥1 be an integer. If r∈Gi and piK∤r, then
1≤j≤dmaxvpj(r)=vpi(r)<K.
Consequently,
{r∈Gi:piK∤r}⊂{r∈R:1≤j≤dmaxvpj(r)<K}.
The set on the right is finite by assumption. Hence there exists NK≥1 such that for any r∈Gi, r≥NK, we have piK∣r.
Now suppose that Gi is infinite. For every N≥NK, the set {r∈Gi:r≥N} is nonempty, and all its elements are divisible by piK. Therefore
piK∣gcd{r∈Gi:r≥N},
and in particular,
gcd{r∈Gi:r≥N}≥piK(N≥NK).
Since K is arbitrary, we obtain
N→∞limgcd{r∈Gi:r≥N}=∞.
Finally, let F be the union of the finite sets among G1,…,Gd, and denote the remaining sets by E1,…,Es. Since R is infinite, at least one Gi is infinite, so 1≤s≤d. Thus
R=F∪E1∪⋯∪Es,
where F is finite and each Ei is infinite and satisfies
N→∞limgcd{r∈Ei:r≥N}=∞.
Corollary 4.2. Let l≥1, let a1,…,al be positive integers, and put
S={a1n1⋯alnl:n1,…,nl∈N0}.
There exist an invertible weakly mixing probability-preserving system (X,B,μ,T) and a Borel set A⊂X such that
Next, choose a prime q∈/P. By the definition of SP, we have q∤r for every r∈SP. Hence, for each r∈SP, there exists an integer b with 1≤b≤q−1 such that r≡b(modq). Consequently,
To prove Corollary 4.2, choose a finite nonempty set of primes Q such that every aj can be written as
aj=p∈Q∏pej,p,ej,p∈N0.
For any n1,…,nl∈N0, we have
a1n1⋯alnl=p∈Q∏p∑j=1lnjej,p∈SQ.
Thus S⊂SQ. By Theorem 1.1, there exist an invertible weakly mixing system (X,B,μ,T) and a Borel set A such that
μ(A)>0,A∩T−rA=∅(r∈SQ).
Since S⊂SQ, the same conclusion holds for every r∈S. □
An infinitely generated semigroup
Corollary 4.3. Let ℓ1<ℓ2<⋯ be the primes greater than 5, and let Γ be the multiplicative semigroup generated by
2,3,2jℓj(j≥1),
including 1. Then there exist an invertible weakly mixing probability-preserving system (X,B,μ,T) and a Borel set A⊂X such that
μ(A)>0,A∩T−rA=∅(r∈Γ).
The system can be chosen as a finite product of two-sided complex Gaussian shifts. Moreover,
{2a3b:a,b∈N0}⊂Γ,2jℓj∈Γ(j≥1).
In particular, Γ is not finitely generated.
Proof. Every r∈Γ can be written as
r=2a3bj≥1∏(2jℓj)cj,
where a,b,cj∈N0 and only finitely many cj are nonzero. Recall that vp(r)=max{k∈N0:pk∣r}. Since each ℓj is a prime greater than 5, we have v2(r)=a+∑j≥1jcj, v3(r)=b.
Fix an integer K≥1. Suppose that max{v2(r),v3(r)}<K. Then a+∑j≥1jcj<K, and b<K. Since all the exponents are nonnegative, we obtain 0≤a,b<K, cj=0 for every j≥K, and 0≤cj<K for every 1≤j<K. Thus r is determined by the K+1 integers a,b,c1,…,cK−1, each having at most K possible values. Consequently,
#{r∈Γ:max{v2(r),v3(r)}<K}≤KK+1<∞.
Since Γ is infinite, applying Lemma 4.1 with p1=2 and $p_2 = 3 gives
Γ=F∪E1∪⋯∪Es,
where F is finite, 1≤s≤2, and each Ei is infinite and satisfies
N→∞limgcd{r∈Ei:r≥N}=∞.
Next, since 2,3,ℓj are all different from 5, we have 5∤r for every r∈Γ. Hence
∣e(r/5)−1∣≥2sin(π/5)>0for any r∈Γ.
Thus (2) holds with
m=1,α1=51,δ=2sin(π/5).
Theorem 1.2 now gives the required system and Borel set.
Finally, since 2,3∈Γ, we have {2a3b:a,b∈N0}⊂Γ. Moreover, ℓj∣2jℓj∈Γ for any j≥1. If Γ were generated by finitely many positive integers b1,…,bt, every ℓj would divide b1⋯bt, which is impossible since the primes ℓj are all distinct. Therefore Γ is not finitely generated. □
Integer translates
We use the following consequence of [8 Theorems 1.1 and 2.6, and Section 3]. The proof of Grivaux’s Theorem 1.1 uses the Hilbert-space operator construction of Eisner and Grivaux [6 Theorem 2.1].
Lemma 4.4. Let Q⊂N be infinite with 1∈Q. Suppose there exist unit complex numbers ζ and λk=1, k≥1, such that
r∈Qinf∣ζr−1∣>0,k→∞limr∈Qsup∣λkr−1∣=0.
Then there exist an invertible weakly mixing probability-preserving system (X,B,μ,T) and a Borel set A⊂X satisfying
μ(A)>0,A∩T−rA=∅(r∈Q).
Corollary 4.5. Let P={p1,…,pd} be a finite nonempty set of primes, let h∈Z, and put
SP={p1n1⋯pdnd:n1,…,nd∈N0}.
There exist an invertible weakly mixing probability-preserving system (X,B,μ,T) and a Borel set A⊂X such that
μ(A)>0,A∩T−rA=∅(r∈(SP+h)∩N).
The system and the set may depend on h.
Proof. For h=0, the conclusion follows from Theorem 1.1. Suppose h=0. By Lemma 4.1, write SP=F∪E1∪⋯∪Es, where F is finite and each Ei is infinite and satisfies
N→∞limgcd{r∈Ei:r≥N}=∞.
For each 1≤i≤s, choose integers ci>∣h∣ and Li>∣h∣ such that
ci∣r(r∈Ei,r≥Li).
Put Ei′=Ei∩[Li,∞). Each Ei′ is infinite and still satisfies the same condition on greatest common divisors. Apply Lemma 3.1 to Ei′ with η=1. We obtain Ei′=Ci,0⊔Ci,1 and unit complex numbers λi,ϵ,k=1 such that
λi,ϵ,k→1,r∈Ci,ϵsupλi,ϵ,kr−1→0
as k→∞, for ϵ=0,1.
Fix i and ϵ, and define Qi,ϵ=(Ci,ϵ+h)∪{1}. Since Li>∣h∣, all elements of Ci,ϵ+h are positive. Moreover, Qi,ϵ is infinite and contains 1. For every r∈Ci,ϵ,
Thus Qi,ϵ satisfies the assumptions of Lemma 4.4. We obtain an invertible weakly mixing system and a positive-measure Borel set with no returns at times in Qi,ϵ.
The remaining positive times belong to the finite set
Lemma 2.3 gives the required system and Borel set. □
Remark 4.6. The proof of Corollary 4.5 also gives a more general result. Suppose
R=F∪E1∪⋯∪Es⊂N,
where F is finite, each Ei is infinite, and
N→∞limgcd{r∈Ei:r≥N}=∞(1≤i≤s).
Then, for every h∈Z∖{0}, there exist an invertible weakly mixing system (X,B,μ,T) and a Borel set A such that
μ(A)>0,A∩T−rA=∅(r∈(R+h)∩N).
Indeed, for each i, we can choose ci>∣h∣ and Li>∣h∣ such that
ci∣r(r∈Ei,r≥Li).
Hence
∣e((r+h)/ci)−1∣=∣e(h/ci)−1∣>0.
The argument used to prove Corollary 4.5 also applies to these sets. We use an additional Gaussian shift to rule out returns at the remaining finitely many times, and then take the product of all the systems.
A compact symbolic realization
A homeomorphism S of a compact metric space Y is topologically transitive if for any nonempty open sets U,V⊂Y, some n≥0 satisfies U∩S−nV=∅. It is topologically weakly mixing if S×S is topologically transitive on Y×Y. A set is clopen if it is both open and closed. Theorem 1.1 also gives the following result for symbolic systems.
Proposition 4.7. Let P={p1,…,pd} be a finite nonempty set of primes, and put
SP={p1n1⋯pdnd:n1,…,nd∈N0}.
There exist a compact set Y⊂{0,1}Z with S(Y)=Y for the shift (Sy)n=yn+1, and a nonempty clopen set U⊂Y, such that
U∩S−rU=∅(r∈SP).
The shift on Y is topologically weakly mixing and admits a full-support weakly mixing invariant Borel probability measure.
Proof. Take (X,B,μ,T) and A from Theorem 1.1. Define
Φ(x)n=1A(Tnx),m=Φ∗μ,Y=suppm.
Since Φ∘T=S∘Φ and T∗μ=μ, we have S∗m=m and S(Y)=Y. Moreover, applying (3) to f∘Φ and g∘Φ shows that (Y,m,S) is weakly mixing. For the clopen set U={y∈Y:y0=1},
m(U)=μ(A)>0,
m(U∩S−rU)=μ(A∩T−rA)=0(r∈SP).
Each U∩S−rU is open in Y, so full support makes it empty. To check topological weak mixing, take nonempty open sets U1,U2,V1,V2⊂Y. Since m has full support, we have ci:=m(Ui)m(Vi)>0. By (3),
There is therefore a common n for which both intersections have positive measure. Since open rectangles form a base for Y×Y, this proves topological transitivity of S×S. □
The author would like to thank his advisor, Professor Siming Tu, for his continued guidance, support, and encouragement. The author is also grateful to Professor Bryna Kra for sharing her earlier unpublished notes and for drawing attention to related results in the literature.
Statement on the Use of AI Tools in This Work: While preparing this work, the author used ChatGPT 6 for assistance with mathematical discussions and editorial revisions. All mathematical results, proofs, and interpretations were verified and approved by the author, who takes full responsibility for the content of this work.
References
(Z. Liu) School of Mathematics (Zhuhai), Sun Yat-sen University, Zhuhai, Guangdong, 519000, P.R. China
[1]E. M. Ackelsberg, Rigidity, weak mixing, and recurrence in abelian groups, Discrete Contin. Dyn. Syst. 42 (2022), no. 4, 1669–1705. doi:10.3934/dcds.2021168.DOI
[2]C. Badea and S. Grivaux, Kazhdan constants, continuous probability measures with large Fourier coefficients and rigidity sequences, Comment. Math. Helv. 95 (2020), no. 1, 99–127. doi:10.4171/CMH/482.DOI
[3]V. Bergelson, Ergodic Ramsey theory—an update, in Ergodic Theory of ℤᵈ Actions (M. Pollicott and K. Schmidt, eds.), London Math. Soc. Lecture Note Ser. 228, Cambridge Univ. Press, Cambridge, 1996, 1–61.
[4]V. Bergelson, A. del Junco, M. Lemańczyk, and J. Rosenblatt, Rigidity and non-recurrence along sequences, Ergodic Theory Dynam. Systems 34 (2014), no. 5, 1464–1502. doi:10.1017/etds.2013.5.DOI
[5]I. P. Cornfeld, S. V. Fomin, and Ya. G. Sinai, Ergodic Theory, Grundlehren der mathematischen Wissenschaften 245, Springer-Verlag, New York, 1982. doi:10.1007/978-1-4615-6927-5.DOI
[6]T. Eisner and S. Grivaux, Hilbertian Jamison sequences and rigid dynamical systems, J. Funct. Anal. 261 (2011), no. 7, 2013–2052. doi:10.1016/j.jfa.2011.06.001.DOI
[7]N. Frantzikinakis, B. Host, and B. Kra, Bohr recurrence and density of non-lacunary semigroups of ℕ, Proc. Amer. Math. Soc. 153 (2025), no. 1, 181–192. doi:10.1090/proc/17006.DOI
[8]S. Grivaux, Non-recurrence sets for weakly mixing linear dynamical systems, Ergodic Theory Dynam. Systems 34 (2014), no. 1, 132–152. doi:10.1017/etds.2012.116.
[9]A. S. Kechris, Global Aspects of Ergodic Group Actions, Mathematical Surveys and Monographs, vol. 160, American Mathematical Society, Providence, RI, 2010. doi:10.1090/surv/160.DOI
[10]F. Maucourant, A nonhomogeneous orbit closure of a diagonal subgroup, Ann. of Math. (2) 171 (2010), no. 1, 557–570. doi:10.4007/annals.2010.171.557.
Olayemi Adeyemi, Ron Buckmire, Ranthony A. Clark, Shanzhen Gao, Jakini Kauba, Lakeshia Legette-Jones, Apoorva Mate, Omayra Ortega, José Pabón, Robin T. Wilson ·