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Weak mixing and non-recurrence along finitely generated multiplicative semigroups of N\mathbb N

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Abstract

Let P\mathcal P be a finite nonempty set of primes, and let SPS_{\mathcal P} be the multiplicative semigroup that they generate. We prove that there are an invertible weakly mixing measure-preserving transformation TT and a set AA of positive measure such that A∩T−rA=∅A\cap T^{-r}A=\varnothing for every r∈SPr\in S_{\mathcal P}. This gives a negative answer to Bergelson's 1996 question concerning recurrence along {2m3n:m,n≥1}\{2^m3^n:m,n\geq1\}, 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 SPS_{\mathcal P} with P\mathcal 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,…}\mathbb{N}=\{1,2,\ldots\} and N0={0,1,2,…}\mathbb{N}_0=\{0,1,2,\ldots\}. A set R⊂NR\subset\mathbb{N} is a set of measurable recurrence if, for every invertible measure-preserving system (X,B,μ,T)(X,\mathcal{B},\mu,T) and every A∈BA\in\mathcal{B} with μ(A)>0\mu(A)>0, there is an r∈Rr\in R such that μ(A∩T−rA)>0\mu(A\cap T^{-r}A)>0.

Consider the multiplicative semigroup R2,3={2m3n:m,n≥1}R_{2,3}=\{2^m3^n:m,n\ge1\}. Since none of its elements is divisible by 5, rotation by 1 on Z/5Z\mathbb{Z}/5\mathbb{Z} shows that R2,3R_{2,3} 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 AA of positive measure satisfy

μ(A∩T−2m3nA)>0for some m,n≥1.\mu(A\cap T^{-2^m3^n}A)>0\qquad\text{for some }m,n\ge1.

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 R2,3R_{2,3} 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}\{k!2^m3^n:k,m,n\ge1\} 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}\mathcal{P}=\{p_1,\ldots,p_d\} be a finite nonempty set of primes and put

SP={p1n1⋯pdnd:n1,…,nd∈N0}.S_{\mathcal{P}}=\{p_1^{n_1}\cdots p_d^{n_d}:n_1,\ldots,n_d\in\mathbb{N}_0\}.

There exist a standard nonatomic probability space (X,B,μ)(X,\mathcal{B},\mu), an invertible weakly mixing probability-preserving transformation T:X→XT:X\to X, and a Borel set A⊂XA\subset X such that μ(A)>0\mu(A)>0 and A∩T−rA=∅A\cap T^{-r}A=\varnothing for every r∈SPr\in S_{\mathcal{P}}.

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 SPS_{\mathcal{P}}, since only finitely many primes divide its generators. Thus the theorem applies to all such semigroups, including the time 1. Taking P={2,3}\mathcal{P}=\{2,3\} answers Bergelson’s question. Coding the set AA also gives a compact topologically weakly mixing subshift with a nonempty clopen set having no return at any time in SPS_{\mathcal{P}}; see Proposition 4.7.

Our argument also applies to sets involving infinitely many distinct primes. Write T=R/Z\mathbb{T}=\mathbb{R}/\mathbb{Z} and e(t)=exp⁡(2πit)e(t)=\exp(2\pi it). A set R⊂NR\subset\mathbb{N} is Bohr recurrent if, for every m≥1m\ge1, α1,…,αm∈T\alpha_1,\ldots,\alpha_m\in\mathbb{T}, and ε>0\varepsilon>0, there exists r∈Rr\in R such that max⁡1≤a≤m∣e(rαa)−1∣<ε\max_{1\le a\le m}|e(r\alpha_a)-1|<\varepsilon. For a nonempty set H⊂NH\subset\mathbb{N}, gcd⁡H\gcd H denotes the greatest positive integer dividing every member of HH. We first prove the following general theorem.

Theorem 1.2. Let R⊂NR\subset\mathbb{N} be of the form

R=F∪E1∪⋯∪Ed,R=F\cup E_1\cup\cdots\cup E_d,

where d≥1d\ge1, FF is finite, and E1,…,EdE_1,\ldots,E_d are infinite. Suppose that

lim⁡N→∞gcd⁡{r∈Ei:r≥N}=∞(1≤i≤d).(1)\lim_{N\to\infty}\gcd\{r\in E_i:r\ge N\}=\infty\qquad(1\le i\le d). \tag*{(1)}

Suppose also that there are α1,…,αm∈T\alpha_1,\ldots,\alpha_m\in\mathbb{T}, with m≥1m\ge1, and δ>0\delta>0 such that

max⁡1≤a≤m∣e(rαa)−1∣≥δ(r∈R).(2)\max_{1\le a\le m}|e(r\alpha_a)-1|\ge\delta\qquad(r\in R). \tag*{(2)}

Then there exist a standard nonatomic probability space (X,B,μ)(X,\mathcal{B},\mu), an invertible weakly mixing probability-preserving transformation T:X→XT:X\to X, and a Borel set A⊂XA\subset X such that μ(A)>0\mu(A)>0, A∩T−rA=∅A\cap T^{-r}A=\varnothing (r∈R)(r\in 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 EiE_i. Condition (2) says that RR 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 SPS_{\mathcal{P}}, assign each integer to a prime with maximal exponent. The resulting sets satisfy (1), and a prime outside P\mathcal{P} gives (2). Section 4 also gives an infinitely generated example and proves non-recurrence for (SP+h)∩N(S_{\mathcal{P}+h})\cap\mathbb{N} for every fixed h∈Zh\in\mathbb{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⊂NQ\subset\mathbb{N} containing 11, one requires unit complex numbers λk≠1\lambda_k\ne1 such that sup⁡r∈Q∣λkr−1∣→0\sup_{r\in Q}|\lambda_k^r-1|\to0. 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 11 within each group. This convergence alone does not ensure that

∑r∈Q∫T∣e(rt)−1∣2 dν(t)\sum_{r\in Q}\int_{\mathbb{T}}|e(rt)-1|^2\,d\nu(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 SPS_{\mathcal{P}}. 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\eta> 0, to be chosen sufficiently small below, and one part EE. Choose denominators DjD_j and integers 1=N0<N1<N2<⋯1 = N_0 < N_1 < N_2 < \cdots in the order D1,N1,D2,N2,…D_1, N_1, D_2, N_2, \ldots, so that DjD_j divides every r∈Er \in E with r≥Njr \ge N_j. For ϵ=0,1\epsilon= 0, 1, let QϵQ_\epsilon consist of those r∈Er \in E lying in an interval [Nj,Nj+1)[N_j, N_{j+1}) with j≡ϵ(mod2)j \equiv\epsilon\pmod{2}. For each QϵQ_\epsilon, consider the random series

Θϵ=∑ℓ≥1ℓ≡ϵ(mod2)ωℓDℓ,ϵ=0,1,\Theta_\epsilon= \sum_{\substack{\ell\ge1 \\ \ell\equiv\epsilon\pmod{2}}} \frac{\omega_\ell}{D_\ell}, \qquad\epsilon= 0, 1,

where the digits ωℓ\omega_\ell are independent, each equal to 0 or 1 with probability 1/21/2. We take the sums modulo one. Choose the denominators large enough and make them grow fast enough that, for each ϵ\epsilon, different choices of the digits used in Θϵ\Theta_\epsilon give different points of T\mathbb{T}. Each such digit sequence has probability zero, so the distribution of each series has no atoms.

Now take r∈Qϵ∩[Nj,Nj+1)r \in Q_\epsilon\cap[N_j, N_{j+1}), so that j≡ϵ(mod2)j \equiv\epsilon\pmod{2}. The denominators of the terms of Θϵ\Theta_\epsilon with indices at most jj divide rr. After multiplication by rr, these terms are integers. They therefore do not change the value of e(rΘϵ)e(r\Theta_\epsilon), which depends only on the remaining terms. Since j+1j+1 has the opposite parity, the remaining terms have indices j+2,j+4,…j+2, j+4, \ldots.

When we choose Dj+2D_{j+2}, the endpoint Nj+1N_{j+1} is already fixed, and every rr in the interval satisfies r<Nj+1r < N_{j+1}. We can therefore choose Dj+2D_{j+2} and the later denominators large enough to make ∣e(rΘϵ)−1∣|e(r\Theta_\epsilon)-1| as small as needed, uniformly for all r∈Qϵ∩[Nj,Nj+1)r \in Q_\epsilon\cap[N_j, N_{j+1}) and all choices of the digits. Since there are finitely many such rr, 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\eta. 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\eta> 0, we obtain a finite partition of SPS_{\mathcal{P}} and, for each part QQ, a continuous probability measure ν\nu on T\mathbb{T} such that

∑r∈Qsup⁡t∈supp⁡ν∣e(rt)−1∣2<η.\sum_{r\in Q}\sup_{t\in\operatorname{supp}\nu}|e(rt)-1|^2 < \eta.

The partition and measures may depend on η\eta.

We now use this estimate to build a weakly mixing system with no returns along QQ. Take a prime q∉Pq \notin\mathcal{P} and put ζ=e(1/q)\zeta=e(1/q). No element of SPS_{\mathcal{P}} is divisible by qq. Hence there is a constant δ>0\delta> 0 such that ∣ζr−1∣≥δ|\zeta^r-1| \ge\delta for all r∈SPr \in S_{\mathcal{P}}. Translate ν\nu by 1/q1/q to obtain a continuous probability measure σ\sigma. Let (X,μ,T)(X,\mu,T) be the complex Gaussian shift associated with σ\sigma, with coordinates Zk=Z0∘TkZ_k=Z_0\circ T^k. The shift is invertible and weakly mixing. Its coordinates satisfy

E∣Zr−ζrZ0∣2=∫T∣e(rt)−1∣2 dν(t).\mathbb{E}|Z_r-\zeta^r Z_0|^2=\int_{\mathbb{T}}|e(rt)-1|^2\,d\nu(t).

Thus the sum of these mean square errors over r∈Qr \in Q is less than η\eta.

Set a=δ/8a=\delta/8 and let C={∣Z0−1∣<a}C=\{|Z_0-1|<a\}. Since Z0Z_0 is standard complex Gaussian, μ(C)>0\mu(C)>0 depends only on aa, not on ν\nu. On C∩T−rCC\cap T^{-r}C, we have ∣Z0−1∣<a,∣Zr−1∣<a|Z_0-1|<a,|Z_r-1|<a. Together with ∣ζr−1∣≥δ|\zeta^r-1|\ge\delta, this gives ∣Zr−ζrZ0∣>δ−2a>δ/2|Z_r-\zeta^r Z_0|>\delta-2a>\delta/2. By Markov's inequality,

∑r∈Qμ(C∩T−rC)≤4δ2∑r∈QE∣Zr−ζrZ0∣2<4ηδ2.\sum_{r\in Q}\mu(C\cap T^{-r}C)\le\frac{4}{\delta^2}\sum_{r\in Q}\mathbb{E}|Z_r-\zeta^r Z_0|^2<\frac{4\eta}{\delta^2}.

Since μ(C)\mu(C) depends only on aa, we apply the preceding construction with η\eta small enough that 4η/δ2<μ(C)/24\eta/\delta^2<\mu(C)/2.

Remove from CC all points that return to CC at a time in Q\mathbb{Q}, and set A=C∖⋃r∈QT−rCA=C\setminus\bigcup_{r\in\mathbb{Q}}T^{-r}C. The sum bound gives μ(A)>μ(C)/2>0\mu(A)>\mu(C)/2>0. Also, A⊂CA\subset C and A∩T−rC=∅A\cap T^{-r}C=\varnothing for every r∈Qr\in\mathbb{Q}. Therefore A∩T−rA=∅A\cap T^{-r}A=\varnothing for all r∈Qr\in\mathbb{Q}. The bound on the sum is needed because we remove the return events for all r∈Qr\in\mathbb{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∈SPr\in S_{\mathcal{P}} belongs to one part. The set in that coordinate has no return at time rr, 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 11, 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)(X,\mathcal{B},\mu) consists of a set XX, a σ\sigma-algebra B\mathcal{B}, and a countably additive measure with μ(X)=1\mu(X)=1. We work with standard Borel spaces: these are measurable spaces isomorphic to a complete separable metric space with its Borel σ\sigma-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\mathbb{T} is called continuous when it has no atoms.

For a measurable map f:X→Yf:X\to Y, its pushforward is (f∗μ)(B)=μ(f−1(B))(f_*\mu)(B)=\mu(f^{-1}(B)). For every nonnegative measurable function hh, and every integrable hh,

∫Yh d(f∗μ)=∫Xh∘f dμ.\int_Y h\,d(f_*\mu)=\int_X h\circ f\,d\mu.

For a Borel probability measure on a separable metric space, its support is

supp⁡μ={x:μ(V)>0 for every open neighbourhood V of x}.\operatorname{supp}\mu=\{x:\mu(V)>0\text{ for every open neighbourhood }V\text{ 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 XX if every nonempty open subset of XX has positive measure. We write 1A\mathbf{1}_A for the indicator of AA.

An invertible measure-preserving system (X,B,μ,T)(X,\mathcal{B},\mu,T) consists of a probability space and a measurable bijection T:X→XT:X\to X with measurable inverse and T∗μ=μT_*\mu=\mu. For r∈Zr\in\mathbb{Z}, we use T−rA={x:Trx∈A}T^{-r}A=\{x:T^r x\in A\}. The transformation is ergodic if μ(T−1A△A)=0\mu(T^{-1}A\mathbin{\triangle}A)=0 implies μ(A)∈{0,1}\mu(A)\in\{0,1\}, where △\triangle denotes symmetric difference. It is weakly mixing if, for all bounded measurable complex functions f,gf,g,

1N∑n=1N∣∫f(g∘Tn) dμ−∫f dμ∫g dμ∣⟶0.(3)\frac{1}{N}\sum_{n=1}^{N}\left|\int f(g\circ T^n)\,d\mu-\int f\,d\mu\int g\,d\mu\right|\longrightarrow0. \tag*{(3)}

Equivalently, T×TT\times T is ergodic for μ×μ\mu\times\mu; see [5]. Taking indicators gives the equivalent set formulation with μ(A∩T−nB)−μ(A)μ(B)\mu(A\cap T^{-n}B)-\mu(A)\mu(B).

For a Borel probability measure σ\sigma on T\mathbb{T}, write

σ^(n)=∫Te(nt) dσ(t)(n∈Z).\widehat{\sigma}(n)=\int_{\mathbb{T}}e(nt)\,d\sigma(t)\qquad(n\in\mathbb{Z}).

Then σ^(0)=1\widehat{\sigma}(0)=1 and σ^(−n)=σ^(n)‾\widehat{\sigma}(-n)=\overline{\widehat{\sigma}(n)}. For a topological space XX, we write B(X)\mathcal{B}(X) for its Borel σ\sigma-algebra. All sequence spaces below carry the product topology, with C\mathbb{C} carrying its usual topology and {0,1}\{0,1\} the discrete topology.

Random variables and Gaussian shifts

Let (Ω,F,ρ)(\Omega,\mathcal{F},\rho) be a probability space. A complex random variable is a measurable map W:Ω→CW:\Omega\to\mathbb{C}. For integrable WW, write EρW=∫ΩW dρ\mathbb{E}_{\rho}W=\int_{\Omega}W\,d\rho, omitting the subscript when the measure is clear. The distribution of a random vector W:Ω→CmW:\Omega\to\mathbb{C}^{m} is the pushforward measure W∗ρW_{*}\rho.

A standard complex Gaussian random variable is a random variable of the form

Z=X+iY2,Z=\frac{X+iY}{\sqrt{2}},

where XX and YY are independent real random variables with density (2π)−1/2e−t2/2(2\pi)^{-1/2}e^{-t^{2}/2} on R\mathbb{R}. The density of ZZ with respect to Lebesgue area measure on C\mathbb{C} is π−1e−∣z∣2\pi^{-1}e^{-|z|^{2}}. In particular,

EZ=EZ2=0,E∣Z∣2=1.\mathbb{E}Z=\mathbb{E}Z^{2}=0,\qquad\mathbb{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\sigma be a Borel probability measure on T\mathbb{T}. There exists a Borel probability measure γσ\gamma_{\sigma} on CZ\mathbb{C}^{\mathbb{Z}} such that the coordinate functions Zk(z)=zkZ_k(z)=z_k, k∈Zk\in\mathbb{Z}, are standard complex Gaussian random variables satisfying

E(ZkZl‾)=σ^(k−l),\mathbb{E}(Z_k\overline{Z_l})=\widehat{\sigma}(k-l),
E(ZkZl)=0(k,l∈Z).\mathbb{E}(Z_k Z_l)=0\qquad(k,l\in\mathbb{Z}).

The measure γσ\gamma_{\sigma} has no atoms. The shift

T:CZ→CZ,(Tz)k=zk+1,T:\mathbb{C}^{\mathbb{Z}}\to\mathbb{C}^{\mathbb{Z}},\qquad(Tz)_k=z_{k+1},

is invertible and preserves γσ\gamma_{\sigma}. If σ\sigma has no atoms, then (CZ,γσ,T)(\mathbb{C}^{\mathbb{Z}},\gamma_{\sigma},T) is weakly mixing.

Proof. Set φ(n)=σ^(n)\varphi(n)=\widehat{\sigma}(n), for any n∈Zn\in\mathbb{Z}. Since σ\sigma is a probability measure, φ(0)=1\varphi(0)=1. Moreover, for any n1,…,nm∈Zn_1,\ldots,n_m\in\mathbb{Z} and c1,…,cm∈Cc_1,\ldots,c_m\in\mathbb{C},

∑a,b=1mca‾cbφ(nb−na)=∫T∣∑b=1mcbe(nbt)∣2 dσ(t)≥0.\sum_{a,b=1}^{m}\overline{c_a}c_b\varphi(n_b-n_a) =\int_{\mathbb{T}}\left|\sum_{b=1}^{m}c_b e(n_b t)\right|^{2}\,d\sigma(t)\geq0.

Thus φ\varphi is positive definite, and [1 Theorem 2.3] applies.

That theorem gives a Borel probability measure γσ\gamma_{\sigma} on CZ\mathbb{C}^{\mathbb{Z}}, invariant under the shift (Sz)k=zk−1(Sz)_k=z_{k-1}. The coordinate functions Zk(z)=zkZ_k(z)=z_k satisfy

EZk=0,\mathbb{E}Z_k=0,
E(ZkZl‾)=φ(k−l)=σ^(k−l),(k,l∈Z),\mathbb{E}(Z_k\overline{Z_l})=\varphi(k-l)=\widehat{\sigma}(k-l),\qquad(k,l\in\mathbb{Z}),
E(ZkZl)=0.\mathbb{E}(Z_kZ_l)=0.

Since these variables are Gaussian and σ^(0)=1\widehat{\sigma}(0)=1, each ZkZ_k is standard complex Gaussian. Define T=S−1T=S^{-1}. Then (Tz)k=zk+1(Tz)_k=z_{k+1}. Since SS is invertible and preserves γσ\gamma_{\sigma}, so does TT.

Since Z0Z_0 is standard complex Gaussian, it has density π−1e−∣w∣2\pi^{-1}e^{-|w|^{2}} on C\mathbb{C}. Thus γσ({Z0=a})=0\gamma_{\sigma}(\{Z_0=a\})=0 for every a∈Ca\in\mathbb{C}. For every z=(zk)k∈Z∈CZz=(z_k)_{k\in\mathbb{Z}}\in\mathbb{C}^{\mathbb{Z}}, we have {z}⊂{w∈CZ:Z0(w)=z0}\{z\}\subset\{w\in\mathbb{C}^{\mathbb{Z}}:Z_0(w)=z_0\} and hence γσ({z})≤γσ({Z0=z0})=0\gamma_{\sigma}(\{z\})\leq\gamma_{\sigma}(\{Z_0=z_0\})=0. Therefore γσ\gamma_{\sigma} has no atoms.

Finally, suppose that σ\sigma has no atoms. By [1 Proposition 2.5], the Gaussian system associated with σ\sigma, namely (CZ,γσ,S)(\mathbb{C}^{\mathbb{Z}},\gamma_{\sigma},S), is weakly mixing. Since weak mixing is preserved under inversion, (CZ,γσ,T)(\mathbb{C}^{\mathbb{Z}},\gamma_{\sigma},T) is also weakly mixing. □

We call (CZ,γσ,T)(\mathbb{C}^{\mathbb{Z}},\gamma_{\sigma},T) the complex Gaussian shift associated with σ\sigma. For later use, note that Z0∘Tn=ZnZ_{0}\circ T^{n}=Z_{n}, so

∫(Z0∘Tn)Z0‾ dγσ=σ^(n)(n∈Z).\int(Z_{0}\circ T^{n})\overline{Z_{0}}\,d\gamma_{\sigma}=\widehat{\sigma}(n)\qquad(n\in\mathbb{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⊂NQ\subset\mathbb{N} be nonempty, and suppose that ζ∈C\zeta\in\mathbb{C} and δ>0\delta>0 satisfy

∣ζ∣=1,∣ζr−1∣≥δ(r∈Q).|\zeta|=1,\qquad|\zeta^{r}-1|\geq\delta\qquad(r\in Q).

Set

a=δ8,cδ=a2e−(1+a)2.a=\frac{\delta}{8},\qquad c_{\delta}=a^{2}e^{-(1+a)^{2}}.

Suppose there is a continuous Borel probability measure ν\nu on T\mathbb{T} such that

∑r∈Q∫T∣e(rt)−1∣2 dν(t)<δ2cδ8.\sum_{r\in Q}\int_{\mathbb{T}}|e(rt)-1|^{2}\,d\nu(t)<\frac{\delta^{2}c_{\delta}}{8}.

Then there exist an invertible weakly mixing complex Gaussian shift (X,B,μ,T)(X,\mathcal{B},\mu,T) and a Borel set A⊂XA\subset X satisfying

μ(A)>cδ2,A∩T−rA=∅(r∈Q).\mu(A)>\frac{c_{\delta}}{2},\qquad A\cap T^{-r}A=\varnothing\qquad(r\in Q).

Proof. Choose α∈T\alpha\in\mathbb{T} with ζ=e(α)\zeta=e(\alpha). Define a Borel probability measure σ\sigma on T\mathbb{T} by

σ(B)=ν(B−α)\sigma(B)=\nu(B-\alpha)

for every Borel set B⊂TB\subset\mathbb{T}. Since ν\nu is continuous, so is σ\sigma. Moreover,

σ^(r)=∫Te(r(t+α)) dν(t)=ζrν^(r).\widehat{\sigma}(r)=\int_{\mathbb{T}}e(r(t+\alpha))\,d\nu(t)=\zeta^{r}\widehat{\nu}(r).

By Lemma 2.1, let

X=CZ,B=B(CZ),μ=γσ,X=\mathbb{C}^{\mathbb{Z}},\qquad\mathcal{B}=\mathcal{B}(\mathbb{C}^{\mathbb{Z}}),\qquad\mu=\gamma_{\sigma},

and define

T:X→X,(Tz)k=zk+1.T:X\to X,\qquad(Tz)_{k}=z_{k+1}.

Then (X,B,μ,T)(X,\mathcal{B},\mu,T) is an invertible weakly mixing measure preserving system. For k∈Zk\in\mathbb{Z}, let Zk:X→CZ_{k}:X\to\mathbb{C} be the coordinate function Zk(z)=zkZ_{k}(z)=z_{k}. Each ZkZ_{k} is a standard complex Gaussian random variable. In particular,

Z0(Trz)=Zr(z),Eμ(ZrZ0‾)=σ^(r).Z_{0}(T^{r}z)=Z_{r}(z),\qquad\mathbb{E}_{\mu}(Z_{r}\overline{Z_{0}})=\widehat{\sigma}(r).

Since Eμ∣Zr∣2=Eμ∣Z0∣2=1\mathbb{E}_{\mu}|Z_{r}|^{2}=\mathbb{E}_{\mu}|Z_{0}|^{2}=1, we have

Eμ∣Zr−ζrZ0∣2=2−2Re⁡(ζ‾ rEμ(ZrZ0‾))=2−2Re⁡(ζ‾ rσ^(r))=2−2Re⁡ν^(r)=∫T∣e(rt)−1∣2 dν(t).\begin{aligned} \mathbb{E}_{\mu}|Z_{r}-\zeta^{r}Z_{0}|^{2} &=2-2\operatorname{Re}\left(\overline{\zeta}^{\,r}\mathbb{E}_{\mu}(Z_{r}\overline{Z_{0}})\right)\\ &=2-2\operatorname{Re}\left(\overline{\zeta}^{\,r}\widehat{\sigma}(r)\right)\\ &=2-2\operatorname{Re}\widehat{\nu}(r)\\ &=\int_{\mathbb{T}}|e(rt)-1|^{2}\,d\nu(t). \end{aligned}

Let C={x∈X:∣Z0(x)−1∣<a}C=\{x\in X:|Z_0(x)-1|<a\}. Since Z0Z_0 is standard complex Gaussian, it has density π−1e−∣z∣2\pi^{-1}e^{-|z|^2} on C\mathbb{C}. Thus, we have

μ(C)=1π∫∣z−1∣<ae−∣z∣2 dA(z)≥1πe−(1+a)2⋅πa2=a2e−(1+a)2=cδ,\mu(C)=\frac{1}{\pi}\int_{|z-1|<a}e^{-|z|^2}\,dA(z) \geq\frac{1}{\pi}e^{-(1+a)^2}\cdot\pi a^2 =a^2e^{-(1+a)^2}=c_\delta,

where dAdA denotes Lebesgue area measure on C\mathbb{C}.

Fix r∈Qr\in\mathbb{Q}. If x∈C∩T−rCx\in C\cap T^{-r}C, then

∣Z0(x)−1∣<a,∣Zr(x)−1∣<a.|Z_0(x)-1|<a,\qquad|Z_r(x)-1|<a.

Since ∣ζr−1∣≥δ|\zeta^r-1|\geq\delta, we have

∣Zr(x)−ζrZ0(x)∣≥∣ζr−1∣−∣Zr(x)−1∣−∣Z0(x)−1∣>δ−2a=3δ4>δ2.|Z_r(x)-\zeta^rZ_0(x)|\geq|\zeta^r-1|-|Z_r(x)-1|-|Z_0(x)-1| >\delta-2a=\frac{3\delta}{4}>\frac{\delta}{2}.

Thus Markov’s inequality gives

μ(C∩T−rC)≤4δ2E∣Zr−ζrZ0∣2=4δ2∫T∣e(rt)−1∣2 dν(t).\mu(C\cap T^{-r}C)\leq\frac{4}{\delta^2}\mathbb{E}|Z_r-\zeta^rZ_0|^2 =\frac{4}{\delta^2}\int_{\mathbb{T}}|e(rt)-1|^2\,d\nu(t).

Now define

A=C∖⋃r∈QT−rC.A=C\setminus\bigcup_{r\in\mathbb{Q}}T^{-r}C.

By the assumption on ν\nu,

μ(A)≥μ(C)−∑r∈Qμ(C∩T−rC)> cδ−4δ2⋅δ2cδ8=cδ2.\mu(A)\geq\mu(C)-\sum_{r\in\mathbb{Q}}\mu(C\cap T^{-r}C) >\ c_\delta-\frac{4}{\delta^2}\cdot\frac{\delta^2c_\delta}{8} =\frac{c_\delta}{2}.

Finally, A⊂CA\subset C and A∩T−rC=∅A\cap T^{-r}C=\varnothing for every r∈Qr\in\mathbb{Q}. Since T−rA⊂T−rCT^{-r}A\subset T^{-r}C, we obtain

A∩T−rA=∅(r∈Q).A\cap T^{-r}A=\varnothing\qquad(r\in\mathbb{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)(X_j,\mathcal{B}_j,\mu_j,T_j), 1≤j≤l1\leq j\leq l, be finitely many invertible weakly mixing probability-preserving systems, and let (X,B,μ,T)(X,\mathcal{B},\mu,T) be their product. Then TT is invertible, probability preserving, and weakly mixing. If Qj⊂NQ_j\subset\mathbb{N} and Aj∈BjA_j\in\mathcal{B}_j satisfy μj(Aj)>0\mu_j(A_j)>0 and Aj∩Tj−rAj=∅A_j\cap T_j^{-r}A_j=\varnothing for every r∈Qjr\in Q_j, then A=∏j=1lAjA=\prod_{j=1}^{l}A_j satisfies

μ(A)>0,A∩T−rA=∅(r∈⋃j=1lQj).\mu(A)>0,\qquad A\cap T^{-r}A=\varnothing\qquad\left(r\in\bigcup_{j=1}^{l}Q_j\right).

Proof. The product of finitely many weakly mixing systems is weakly mixing; see [4 Section 4]. Moreover,

μ(A)=∏j=1lμj(Aj)>0,A∩T−rA=∏j=1l(Aj∩Tj−rAj).\mu(A)=\prod_{j=1}^{l}\mu_j(A_j)>0,\qquad A\cap T^{-r}A=\prod_{j=1}^{l}(A_j\cap T_j^{-r}A_j).

For r∈⋃j=1ℓQjr \in\bigcup_{j=1}^{\ell} Q_j, there exists jj such that

Aj∩Tj−rAj=∅.A_j \cap T_j^{-r} A_j = \varnothing.

Hence A∩T−rA=∅A \cap T^{-r} A = \varnothing.

Lemma 2.4. For every finite set H⊂NH \subset\mathbb{N}, there are an invertible weakly mixing two-sided complex Gaussian shift (X,B,μ,T)(X,\mathcal{B},\mu,T) and a Borel set BB of positive measure such that B∩T−rB=∅B \cap T^{-r}B = \varnothing for all r∈Hr \in H.

Proof. Take the Gaussian shift in Lemma 2.1, with σ\sigma equal to normalized Lebesgue measure on T\mathbb{T}. Its coordinates are independent standard complex Gaussian variables, and the shift is weakly mixing. Put L=max⁡(H∪{0})L=\max(H\cup\{0\}) and

B={∣Z0−1∣<1/4}∩⋂k=1L{∣Zk∣<1/4}.B=\{|Z_0-1|<1/4\}\cap\bigcap_{k=1}^{L}\{|Z_k|<1/4\}.

By independence and the positivity of the Gaussian density, μ(B)>0\mu(B)>0. For every r∈Hr\in H, if x∈B∩T−rBx\in B\cap T^{-r}B, then

∣Zr(x)∣<1/4,∣Zr(x)−1∣=∣Z0(Trx)−1∣<1/4.|Z_r(x)|<1/4,\qquad|Z_r(x)-1|=|Z_0(T^r x)-1|<1/4.

Hence

1≤∣Zr(x)∣+∣Zr(x)−1∣<1/2,1\leq|Z_r(x)|+|Z_r(x)-1|<1/2,

a contradiction. Thus B∩T−rB=∅B\cap T^{-r}B=\varnothing for all r∈Hr\in 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∣|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⊂NE\subset\mathbb{N} be infinite and suppose that

gcd⁡{r∈E:r≥N}⟶∞(N⟶∞).\gcd\{r\in E:r\geq N\}\longrightarrow\infty\qquad(N\longrightarrow\infty).

Then for every η>0\eta>0, there are a partition E=C0⊔C1E=C_0\sqcup C_1 into infinite sets and continuous Borel probability measures ν0,ν1\nu_0,\nu_1 on T\mathbb{T} such that, with Qϵ=Cϵ∪{1}Q_\epsilon=C_\epsilon\cup\{1\},

∑r∈Qϵsup⁡t∈supp⁡νϵ∣e(rt)−1∣2<η(ϵ=0,1).\sum_{r\in Q_\epsilon}\sup_{t\in\operatorname{supp}\nu_\epsilon}|e(rt)-1|^2<\eta\qquad(\epsilon=0,1).

For each of these fixed sets QϵQ_\epsilon, there are unit complex numbers λϵ,k≠1\lambda_{\epsilon,k}\ne1 satisfying

λϵ,k⟶1,sup⁡r∈Qϵ∣λϵ,k r−1∣⟶0(k⟶∞).(4)\lambda_{\epsilon,k}\longrightarrow1,\qquad\sup_{r\in Q_\epsilon}|\lambda_{\epsilon,k}^{\,r}-1|\longrightarrow0\qquad(k\longrightarrow\infty). \tag*{(4)}

The partition and measures may depend on η\eta.

Proof. For each NN, the integer gcd⁡{r∈E:r≥N}\gcd\{r\in E:r\ge N\} divides all but finitely many members of EE. Hence the hypothesis implies that

D={D∈N:D divides all but finitely many members of E}D=\{D\in\mathbb{N}:D\text{ divides all but finitely many members of }E\}

is unbounded. Set D0=N0=1D_0=N_0=1. After Dj−1D_{j-1} and Nj−1N_{j-1} have been fixed, choose Dj∈DD_j\in D so that

Dj≥4Dj−1,Dj≥2jNj−1,16π2Nj−13Dj2<η2−j(j≥1),D_j\ge4D_{j-1},\qquad D_j\ge2^jN_{j-1},\qquad\frac{16\pi^2N_{j-1}^3}{D_j^2}<\eta2^{-j}\quad(j\ge1),

and then choose an integer Nj>Nj−1N_j>N_{j-1} such that

Dj∣r(r∈E, r≥Nj),E∩[Nj−1,Nj)≠∅.D_j\mid r\quad(r\in E,\ r\ge N_j),\qquad E\cap[N_{j-1},N_j)\ne\varnothing.

Such an NjN_j exists because Dj∈DD_j\in D and EE is unbounded. No divisibility between successive DjD_j is required. Define

Cϵ=E∩⋃j≥0j≡ϵ(mod2)[Nj,Nj+1),Iϵ={ℓ≥1:ℓ≡ϵ(mod2)}.C_\epsilon=E\cap\bigcup_{\substack{j\ge0\\j\equiv\epsilon\pmod2}}[N_j,N_{j+1}),\qquad I_\epsilon=\{\ell\ge1:\ell\equiv\epsilon\pmod2\}.

Every interval meets EE, so E=C0⊔C1E=C_0\sqcup C_1 and both sets are infinite. For ϵ∈{0,1}\epsilon\in\{0,1\}, let Ωϵ={0,1}Iϵ\Omega_\epsilon=\{0,1\}^{I_\epsilon} be equipped with the product probability measure Pϵ\mathbb{P}_\epsilon under which each coordinate takes the values 0 and 1 with equal probability. For ω=(ωℓ)ℓ∈Iϵ∈Ωϵ\omega=(\omega_\ell)_{\ell\in I_\epsilon}\in\Omega_\epsilon, define

Θϵ(ω)=∑ℓ∈IϵωℓDℓ.\Theta_\epsilon(\omega)=\sum_{\ell\in I_\epsilon}\frac{\omega_\ell}{D_\ell}.

We define a probability measure νϵ\nu_\epsilon on T\mathbb{T} by

νϵ(B)=Pϵ{ω∈Ωϵ:Θϵ(ω) mod 1∈B}\nu_\epsilon(B)=\mathbb{P}_\epsilon\{\omega\in\Omega_\epsilon:\Theta_\epsilon(\omega)\bmod1\in B\}

for every Borel set B⊂TB\subset\mathbb{T}. Since Dℓ+1≥4DℓD_{\ell+1}\ge4D_\ell and D1≥4D_1\ge4, we have

0≤Θϵ(ω)≤∑ℓ=1∞1Dℓ≤1D1∑ℓ=0∞4−ℓ=43D1≤12.0\le\Theta_\epsilon(\omega)\le\sum_{\ell=1}^{\infty}\frac{1}{D_\ell}\le\frac{1}{D_1}\sum_{\ell=0}^{\infty}4^{-\ell}=\frac{4}{3D_1}\le\frac12.

The series converges uniformly on the compact space Ωϵ\Omega_\epsilon. Thus Θϵ\Theta_\epsilon is continuous on Ωϵ\Omega_\epsilon. Consequently,

Kϵ={∑ℓ∈IϵωℓDℓ(mod1):ωℓ∈{0,1}}K_\epsilon=\left\{\sum_{\ell\in I_\epsilon}\frac{\omega_\ell}{D_\ell}\pmod1:\omega_\ell\in\{0,1\}\right\}

is compact. By the definition of νϵ\nu_\epsilon, νϵ(Kϵ)=1\nu_\epsilon(K_\epsilon)=1, and supp⁡νϵ⊂Kϵ\operatorname{supp}\nu_\epsilon\subset K_\epsilon.

Let ω≠ω′\omega\ne\omega', and let ℓ∈Iϵ\ell\in I_\epsilon be the first index at which they differ. Then

∣Θϵ(ω)−Θϵ(ω′)∣=∣ωℓ−ωℓ′Dℓ+∑k∈Iϵk>ℓωk−ωk′Dk∣≥1Dℓ−∑k∈Iϵk>ℓ1Dk≥1Dℓ−2Dℓ+2≥78Dℓ>0.\begin{aligned} \left|\Theta_\epsilon(\omega)-\Theta_\epsilon(\omega')\right| &=\left|\frac{\omega_\ell-\omega'_\ell}{D_\ell}+\sum_{\substack{k\in I_\epsilon\\k>\ell}}\frac{\omega_k-\omega'_k}{D_k}\right|\\ &\ge\frac{1}{D_\ell}-\sum_{\substack{k\in I_\epsilon\\k>\ell}}\frac{1}{D_k}\\ &\ge\frac{1}{D_\ell}-\frac{2}{D_{\ell+2}}\ge\frac{7}{8D_\ell}>0. \end{aligned}

Hence, for ω≠ω′\omega\ne\omega', 0<∣Θϵ(ω)−Θϵ(ω′)∣≤12<10<|\Theta_\epsilon(\omega)-\Theta_\epsilon(\omega')|\le\frac12<1. In particular, Θϵ(ω)−Θϵ(ω′)∉Z\Theta_\epsilon(\omega)-\Theta_\epsilon(\omega')\notin\mathbb{Z}. Thus Θϵ(ω)≢Θϵ(ω′)(mod1)\Theta_\epsilon(\omega)\not\equiv\Theta_\epsilon(\omega')\pmod1, and then for every t∈Kϵt\in K_\epsilon, there is a unique ω∈Ωϵ\omega\in\Omega_\epsilon such that

Θϵ(ω)=t(mod1).\Theta_\epsilon(\omega)=t\pmod1.

Finally, we show that νϵ\nu_\epsilon has no atoms. Fix a=(aℓ)ℓ∈Iϵ∈Ωϵa=(a_\ell)_{\ell\in I_\epsilon}\in\Omega_\epsilon. For every integer M≥1M\ge1, independence gives

Pϵ({ω=a})≤Pϵ(ω2i−ϵ=a2i−ϵ for 1≤i≤M)=∏i=1MPϵ(ω2i−ϵ=a2i−ϵ)=2−M.\mathbb{P}_\epsilon(\{\omega=a\})\le\mathbb{P}_\epsilon(\omega_{2i-\epsilon}=a_{2i-\epsilon}\text{ for }1\le i\le M) =\prod_{i=1}^{M}\mathbb{P}_\epsilon(\omega_{2i-\epsilon}=a_{2i-\epsilon})=2^{-M}.

Letting M→∞M \to\infty, we obtain Pϵ({ω=a})=0\mathbb{P}_{\epsilon}(\{\omega=a\})=0. Since ω↦Θϵ(ω)\omega\mapsto\Theta_{\epsilon}(\omega) (mod 1) is injective, for every t∈Tt \in\mathbb{T} the set

{ω∈Ωϵ:Θϵ(ω)≡t(mod1)}\{\omega\in\Omega_{\epsilon}:\Theta_{\epsilon}(\omega)\equiv t \pmod1\}

contains at most one element. Since every singleton in Ωϵ\Omega_{\epsilon} has probability zero, we obtain

νϵ({t})=Pϵ(Θϵ(ω)≡t(mod1))=0.\nu_{\epsilon}(\{t\})=\mathbb{P}_{\epsilon}\bigl(\Theta_{\epsilon}(\omega)\equiv t \pmod1\bigr)=0.

Hence νϵ\nu_{\epsilon} is a continuous probability measure.

Fix r∈E∩[Nj,Nj+1)r \in E \cap[N_j,N_{j+1}), where j≡ϵ(mod2)j \equiv\epsilon\pmod2. For every ℓ∈Iϵ\ell\in I_{\epsilon} with ℓ≤j\ell\le j, we have r≥Nj≥Nℓr \ge N_j \ge N_{\ell}. By the choice of NℓN_{\ell}, Dℓ∣rD_{\ell}\mid r, rωℓDℓ∈Z\frac{r\omega_{\ell}}{D_{\ell}}\in\mathbb{Z}. Since j+1∉Iϵj+1 \notin I_{\epsilon}, it follows that

rΘϵ(ω)=∑ℓ∈Iϵℓ≤jrωℓDℓ+r∑ℓ∈Iϵℓ≥j+2ωℓDℓ≡r∑ℓ∈Iϵℓ≥j+2ωℓDℓ(mod1).r\Theta_{\epsilon}(\omega)=\sum_{\substack{\ell\in I_{\epsilon}\\ \ell\le j}}\frac{r\omega_{\ell}}{D_{\ell}}+r\sum_{\substack{\ell\in I_{\epsilon}\\ \ell\ge j+2}}\frac{\omega_{\ell}}{D_{\ell}} \equiv r\sum_{\substack{\ell\in I_{\epsilon}\\ \ell\ge j+2}}\frac{\omega_{\ell}}{D_{\ell}}\pmod1.

When j=0j=0, we have ϵ=0\epsilon=0 and Iϵ={2,4,6,…}I_{\epsilon}=\{2,4,6,\ldots\}, so the first sum is empty and the same identity holds.

Using ∣e2πiu−1∣≤2π∣u∣\lvert e^{2\pi i u}-1\rvert\le2\pi\lvert u\rvert and 0≤ωℓ≤10\le\omega_{\ell}\le1, we obtain

∣e(rΘϵ(ω))−1∣≤2πr∑ℓ∈Iϵℓ≥j+2ωℓDℓ≤2πr∑ℓ≥j+21Dℓ≤2πrDj+2∑k=0∞4−k≤4πNj+1Dj+2,\begin{aligned} \left\lvert e\bigl(r\Theta_{\epsilon}(\omega)\bigr)-1\right\rvert \le2\pi r\sum_{\substack{\ell\in I_{\epsilon}\\ \ell\ge j+2}}\frac{\omega_{\ell}}{D_{\ell}} \le2\pi r\sum_{\ell\ge j+2}\frac{1}{D_{\ell}} \\ &\le\frac{2\pi r}{D_{j+2}}\sum_{k=0}^{\infty}4^{-k} \le\frac{4\pi N_{j+1}}{D_{j+2}}, \end{aligned}

where the last inequality uses r<Nj+1r<N_{j+1}. Since this estimate holds for every ω∈Ωϵ\omega\in\Omega_{\epsilon}, the definition of KϵK_{\epsilon} gives

sup⁡t∈Kϵ∣e(rt)−1∣≤4πNj+1Dj+2.\sup_{t\in K_{\epsilon}}\lvert e(rt)-1\rvert\le\frac{4\pi N_{j+1}}{D_{j+2}}.

Since the interval contains at most Nj+1N_{j+1} integers,

∑r∈E∩[Nj,Nj+1)sup⁡t∈Kϵ∣e(rt)−1∣2≤16π2Nj+13Dj+22<η2−j−2.\sum_{r\in E\cap[N_j,N_{j+1})}\sup_{t\in K_{\epsilon}}\lvert e(rt)-1\rvert^2 \le\frac{16\pi^2N_{j+1}^3}{D_{j+2}^2}<\eta2^{-j-2}.

Also,

sup⁡t∈Kϵ∣e(t)−1∣2≤16π2D12<η2.\sup_{t\in K_{\epsilon}}\lvert e(t)-1\rvert^2\le\frac{16\pi^2}{D_1^2}<\frac{\eta}{2}.

Combining the estimates for r∈Cϵr\in C_{\epsilon} and r=1r=1, we obtain

∑r∈Cϵ∪{1}sup⁡t∈Kϵ∣e(rt)−1∣2≤∑r∈Cϵsup⁡t∈Kϵ∣e(rt)−1∣2+sup⁡t∈Kϵ∣e(t)−1∣2<η2+η2=η.\begin{aligned} \sum_{r\in C_{\epsilon}\cup\{1\}}\sup_{t\in K_{\epsilon}}\lvert e(rt)-1\rvert^2 \le\sum_{r\in C_{\epsilon}}\sup_{t\in K_{\epsilon}}\lvert e(rt)-1\rvert^2+\sup_{t\in K_{\epsilon}}\lvert e(t)-1\rvert^2 \\ &<\frac{\eta}{2}+\frac{\eta}{2}=\eta. \end{aligned}

Finally, for each J≥2J\ge2 with J≡ϵ(mod2)J\equiv\epsilon\pmod2, define λJ=e(1/DJ)≠1\lambda_J=e(1/D_J)\ne1. For r∈Cϵ∩[Nj,Nj+1)r\in C_{\epsilon}\cap[N_j,N_{j+1}),

{DJ∣r,j≥J,r<NJ−1,j<J,\begin{cases} D_J\mid r, & j\ge J,\\ r<N_{J-1}, & j<J, \end{cases}

because j<Jj<J implies j≤J−2j\le J-2. Hence, including r=1r=1,

sup⁡r∈Qϵ∣λJr−1∣≤2πNJ−1DJ≤2π2−J.\sup_{r\in Q_{\epsilon}}\lvert\lambda_J^r-1\rvert\le\frac{2\pi N_{J-1}}{D_J}\le2\pi2^{-J}.

Since DJ→∞D_J \to\infty, we have λJ→1\lambda_J \to1. Taking J=2k+εJ=2k+\varepsilon and

λε,k=e(1/D2k+ε),k≥1,\lambda_{\varepsilon,k}=e(1/D_{2k+\varepsilon}), \qquad k \ge1,

proves (4). □

Now, we prove our main result.

Proof of Theorem 1.2. Let α1,…,αm∈T\alpha_1,\ldots,\alpha_m \in\mathbb{T} and δ>0\delta>0 satisfy (2), and set

cδ=(δ/8)2exp⁡(−(1+δ/8)2),η=δ2cδ/16.c_\delta=(\delta/8)^2\exp\left(-(1+\delta/8)^2\right), \qquad\eta=\delta^2c_\delta/16.

Apply Lemma 3.1 to each EiE_i, obtaining Ei=Ci,0⊔Ci,1E_i=C_{i,0}\sqcup C_{i,1} and measures νi,ε\nu_{i,\varepsilon}. For r∈Rr\in R, put

a(r)=min⁡{a:∣e(rαa)−1∣≥δ},Ri,ε,a={r∈Ci,ε:a(r)=a}.a(r)=\min\{a:|e(r\alpha_a)-1|\ge\delta\}, \qquad R_{i,\varepsilon,a}=\{r\in C_{i,\varepsilon}:a(r)=a\}.

On each nonempty Ri,ε,aR_{i,\varepsilon,a}, the number ζa=e(αa)\zeta_a=e(\alpha_a) and the measure νi,ε\nu_{i,\varepsilon} satisfy

inf⁡r∈Ri,ε,a∣ζar−1∣≥δ,∑r∈Ri,ε,a∫T∣e(rt)−1∣2 dνi,ε(t)<η<δ2cδ8.\inf_{r\in R_{i,\varepsilon,a}}|\zeta_a^r-1|\ge\delta, \qquad\sum_{r\in R_{i,\varepsilon,a}}\int_{\mathbb{T}}|e(rt)-1|^2\,d\nu_{i,\varepsilon}(t)<\eta<\frac{\delta^2c_\delta}{8}.

Then

R=F∪⋃i=1d⋃ε=01⋃a=1mRi,ε,a.R=F\cup\bigcup_{i=1}^{d}\bigcup_{\varepsilon=0}^{1}\bigcup_{a=1}^{m}R_{i,\varepsilon,a}.

Write the nonempty sets among FF and Ri,ε,aR_{i,\varepsilon,a} as Q1,…,QLQ_1,\ldots,Q_L. Then L≤2dm+1L\le2dm+1. By Proposition 2.2 and Lemma 2.4, for each QjQ_j there is a weakly mixing Gaussian shift (Xj,μj,Tj)(X_j,\mu_j,T_j) and a Borel set AjA_j such that

μj(Aj)>0,Aj∩Tj−rAj=∅(r∈Qj).\mu_j(A_j)>0, \qquad A_j\cap T_j^{-r}A_j=\varnothing\quad(r\in Q_j).

Now set

(X,μ,T)=∏j=1L(Xj,μj,Tj),A=∏j=1LAj.(X,\mu,T)=\prod_{j=1}^{L}(X_j,\mu_j,T_j), \qquad A=\prod_{j=1}^{L}A_j.

By Lemma 2.3, TT is weakly mixing, and

μ(A)=∏j=1Lμj(Aj)>0,A∩T−rA=∅(r∈R).\mu(A)=\prod_{j=1}^{L}\mu_j(A_j)>0, \qquad A\cap T^{-r}A=\varnothing\quad(r\in R).

This completes the proof. □

Remark 3.2. Condition (1) alone does not guarantee non-recurrence. Consider

R∗=⋃k>1{j2k:1≤j≤k}.R_*=\bigcup_{k>1}\{j2^k:1\le j\le k\}.

We first show that R∗R_* is a set of recurrence. Let (X,B,μ,T)(X,\mathcal{B},\mu,T) be an invertible probability-preserving system, and let A∈BA\in\mathcal{B} satisfy μ(A)>0\mu(A)>0. Choose k≥1k\ge1 such that (k+1)μ(A)>1(k+1)\mu(A)>1. Since

∑j=0kμ(T−j2kA)=(k+1)μ(A)>1,\sum_{j=0}^{k}\mu(T^{-j2^k}A)=(k+1)\mu(A)>1,

there exist 0≤i<j≤k0\le i<j\le k such that

μ(T−i2kA∩T−j2kA)>0.\mu(T^{-i2^k}A\cap T^{-j2^k}A)>0.

By invariance of μ\mu,

μ(A∩T−(j−i)2kA)>0.\mu(A\cap T^{-(j-i)2^k}A)>0.

Since (j−i)2k∈R∗(j-i)2^k\in R_*, the set R∗R_* is recurrent; compare [8 Remark 3.1]. On the other hand, for every K≥1K\ge1, all elements of R∗R_* outside the finitely many sets

{j2k:1≤j≤k},1≤k<K,\{j2^k:1\le j\le k\}, \qquad1\le k<K,

are divisible by 2K2^{K}. Hence

lim⁡N→∞gcd⁡{r∈R∗:r≥N}=∞.\lim_{N \to\infty} \gcd\{r \in R_* : r \ge N\} = \infty.

Thus R∗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⊂NR \subset\mathbb{N} be infinite, let p1,…,pdp_1,\ldots,p_d be distinct primes, with d≥1d \ge1, and write vpi(r)=max⁡{k∈N0:pik∣r}v_{p_i}(r) = \max\{k \in\mathbb{N}_0 : p_i^k \mid r\}. Suppose that

#{r∈R:max⁡1≤i≤dvpi(r)<K}<∞for every integer K≥1.\#\{r \in R : \max_{1 \le i \le d} v_{p_i}(r) < K\} < \infty\quad\text{for every integer } K \ge1.

Then R=F∪E1∪⋯∪EsR = F \cup E_1 \cup\cdots\cup E_s, where FF is finite, 1≤s≤d1 \le s \le d, each EiE_i is infinite, and

gcd⁡{r∈Ei:r≥N}⟶∞(N→∞, 1≤i≤s).\gcd\{r \in E_i : r \ge N\} \longrightarrow\infty\quad(N \to\infty,\ 1 \le i \le s).

Proof. For each r∈Rr \in R, choose the smallest index ii for which vpi(r)v_{p_i}(r) is maximal. More precisely, set i(r)=min⁡{i:vpi(r)=max⁡1≤j≤dvpj(r)}i(r) = \min\{i : v_{p_i}(r) = \max_{1 \le j \le d} v_{p_j}(r)\}, Gi={r∈R:i(r)=i}G_i = \{r \in R : i(r) = i\}. Then

R=⋃i=1dGi.R = \bigcup_{i=1}^{d} G_i.

Fix 1≤i≤d1 \le i \le d. We show that if GiG_i is infinite, then

lim⁡N→∞gcd⁡{r∈Gi:r≥N}=∞.\lim_{N \to\infty} \gcd\{r \in G_i : r \ge N\} = \infty.

Let K≥1K \ge1 be an integer. If r∈Gir \in G_i and piK∤rp_i^K \nmid r, then

max⁡1≤j≤dvpj(r)=vpi(r)<K.\max_{1 \le j \le d} v_{p_j}(r) = v_{p_i}(r) < K.

Consequently,

{r∈Gi:piK∤r}⊂{r∈R:max⁡1≤j≤dvpj(r)<K}.\{r \in G_i : p_i^K \nmid r\} \subset\{r \in R : \max_{1 \le j \le d} v_{p_j}(r) < K\}.

The set on the right is finite by assumption. Hence there exists NK≥1N_K \ge1 such that for any r∈Gir \in G_i, r≥NKr \ge N_K, we have piK∣rp_i^K \mid r.

Now suppose that GiG_i is infinite. For every N≥NKN \ge N_K, the set {r∈Gi:r≥N}\{r \in G_i : r \ge N\} is nonempty, and all its elements are divisible by piKp_i^K. Therefore

piK∣gcd⁡{r∈Gi:r≥N},p_i^K \mid\gcd\{r \in G_i : r \ge N\},

and in particular,

gcd⁡{r∈Gi:r≥N}≥piK(N≥NK).\gcd\{r \in G_i : r \ge N\} \ge p_i^K \quad(N \ge N_K).

Since KK is arbitrary, we obtain

lim⁡N→∞gcd⁡{r∈Gi:r≥N}=∞.\lim_{N \to\infty} \gcd\{r \in G_i : r \ge N\} = \infty.

Finally, let FF be the union of the finite sets among G1,…,GdG_1,\ldots,G_d, and denote the remaining sets by E1,…,EsE_1,\ldots,E_s. Since RR is infinite, at least one GiG_i is infinite, so 1≤s≤d1 \le s \le d. Thus

R=F∪E1∪⋯∪Es,R = F \cup E_1 \cup\cdots\cup E_s,

where FF is finite and each EiE_i is infinite and satisfies

lim⁡N→∞gcd⁡{r∈Ei:r≥N}=∞.\lim_{N \to\infty} \gcd\{r \in E_i : r \ge N\} = \infty.

Corollary 4.2. Let l≥1l \ge1, let a1,…,ala_1,\ldots,a_l be positive integers, and put

S={a1n1⋯alnl:n1,…,nl∈N0}.S=\{a_1^{n_1}\cdots a_l^{n_l}:n_1,\ldots,n_l\in\mathbb{N}_0\}.

There exist an invertible weakly mixing probability-preserving system (X,B,μ,T)(X,\mathcal{B},\mu,T) and a Borel set A⊂XA\subset X such that

μ(A)>0,A∩T−rA=∅(r∈S).\mu(A)>0,\qquad A\cap T^{-r}A=\varnothing\quad(r\in S).

Proof of Theorem 1.1 and Corollary 4.2. Let P={p1,…,pd}\mathcal{P}=\{p_1,\ldots,p_d\}. Every r∈SPr\in S_{\mathcal{P}} has a unique representation

r=p1n1⋯pdnd,n1,…,nd∈N0,r=p_1^{n_1}\cdots p_d^{n_d},\qquad n_1,\ldots,n_d\in\mathbb{N}_0,

with vpi(r)=niv_{p_i}(r)=n_i for 1≤i≤d1\le i\le d. For every integer K≥1K\ge1, we therefore have

#{r∈SP:max⁡1≤i≤dvpi(r)<K}=#{(n1,…,nd):0≤ni<K, 1≤i≤d}=Kd<∞.\#\left\{r\in S_{\mathcal{P}}:\max_{1\le i\le d}v_{p_i}(r)<K\right\} =\#\{(n_1,\ldots,n_d):0\le n_i<K,\ 1\le i\le d\}=K^d<\infty.

By Lemma 4.1, we can write

SP=F∪E1∪⋯∪Es,S_{\mathcal{P}}=F\cup E_1\cup\cdots\cup E_s,

where FF is finite, 1≤s≤d1\le s\le d, and each EiE_i is infinite and satisfies

lim⁡N→∞gcd⁡{r∈Ei:r≥N}=∞.\lim_{N\to\infty}\gcd\{r\in E_i:r\ge N\}=\infty.

Thus the first condition of Theorem 1.2 holds.

Next, choose a prime q∉Pq\notin\mathcal{P}. By the definition of SPS_{\mathcal{P}}, we have q∤rq\nmid r for every r∈SPr\in S_{\mathcal{P}}. Hence, for each r∈SPr\in S_{\mathcal{P}}, there exists an integer bb with 1≤b≤q−11\le b\le q-1 such that r≡b(modq)r\equiv b\pmod q. Consequently,

∣e(r/q)−1∣=∣e(b/q)−1∣=2sin⁡(πbq)≥2sin⁡(πq)>0.\left|\mathrm{e}(r/q)-1\right|=\left|\mathrm{e}(b/q)-1\right|=2\sin\left(\frac{\pi b}{q}\right)\ge2\sin\left(\frac{\pi}{q}\right)>0.

Therefore (2) holds with

m=1,α1=1q,δ=2sin⁡(πq).m=1,\qquad\alpha_1=\frac{1}{q},\qquad\delta=2\sin\left(\frac{\pi}{q}\right).

Theorem 1.2 now gives the required system and set, proving Theorem 1.1.

To prove Corollary 4.2, choose a finite nonempty set of primes Q\mathcal{Q} such that every aja_j can be written as

aj=∏p∈Qpej,p,ej,p∈N0.a_j=\prod_{p\in\mathcal{Q}}p^{e_{j,p}},\qquad e_{j,p}\in\mathbb{N}_0.

For any n1,…,nl∈N0n_1,\ldots,n_l\in\mathbb{N}_0, we have

a1n1⋯alnl=∏p∈Qp∑j=1lnjej,p∈SQ.a_1^{n_1}\cdots a_l^{n_l}=\prod_{p\in\mathcal{Q}}p^{\sum_{j=1}^{l}n_je_{j,p}}\in S_{\mathcal{Q}}.

Thus S⊂SQS\subset S_{\mathcal{Q}}. By Theorem 1.1, there exist an invertible weakly mixing system (X,B,μ,T)(X,\mathcal{B},\mu,T) and a Borel set AA such that

μ(A)>0,A∩T−rA=∅(r∈SQ).\mu(A)>0,\qquad A\cap T^{-r}A=\varnothing\quad(r\in S_{\mathcal{Q}}).

Since S⊂SQS\subset S_{\mathcal{Q}}, the same conclusion holds for every r∈Sr\in S. □\square

An infinitely generated semigroup

Corollary 4.3. Let ℓ1<ℓ2<⋯\ell_1 < \ell_2 < \cdots be the primes greater than 5, and let Γ\Gamma be the multiplicative semigroup generated by

2,3,2jℓj(j≥1),2,\quad3,\quad2^j\ell_j\quad(j \ge1),

including 1. Then there exist an invertible weakly mixing probability-preserving system (X,B,μ,T)(X,\mathcal{B},\mu,T) and a Borel set A⊂XA \subset X such that

μ(A)>0,A∩T−rA=∅(r∈Γ).\mu(A) > 0,\qquad A \cap T^{-r}A = \varnothing\quad(r \in\Gamma).

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).\{2^a3^b : a,b \in\mathbb{N}_0\} \subset\Gamma,\qquad2^j\ell_j \in\Gamma\quad(j \ge1).

In particular, Γ\Gamma is not finitely generated.

Proof. Every r∈Γr \in\Gamma can be written as

r=2a3b∏j≥1(2jℓj)cj,r = 2^a3^b \prod_{j \ge1}(2^j\ell_j)^{c_j},

where a,b,cj∈N0a,b,c_j \in\mathbb{N}_0 and only finitely many cjc_j are nonzero. Recall that vp(r)=max⁡{k∈N0:pk∣r}v_p(r) = \max\{k \in\mathbb{N}_0 : p^k \mid r\}. Since each ℓj\ell_j is a prime greater than 5, we have v2(r)=a+∑j≥1jcjv_2(r) = a + \sum_{j \ge1}jc_j, v3(r)=bv_3(r) = b.

Fix an integer K≥1K \ge1. Suppose that max⁡{v2(r),v3(r)}<K\max\{v_2(r),v_3(r)\} < K. Then a+∑j≥1jcj<Ka + \sum_{j \ge1}jc_j < K, and b<Kb < K. Since all the exponents are nonnegative, we obtain 0≤a,b<K0 \le a,b < K, cj=0c_j = 0 for every j≥Kj \ge K, and 0≤cj<K0 \le c_j < K for every 1≤j<K1 \le j < K. Thus rr is determined by the K+1K+1 integers a,b,c1,…,cK−1a,b,c_1,\ldots,c_{K-1}, each having at most KK possible values. Consequently,

#{r∈Γ:max⁡{v2(r),v3(r)}<K}≤KK+1<∞.\#\{r \in\Gamma: \max\{v_2(r),v_3(r)\} < K\} \le K^{K+1} < \infty.

Since Γ\Gamma is infinite, applying Lemma 4.1 with p1=2p_1 = 2 and $p_2 = 3 gives

Γ=F∪E1∪⋯∪Es,\Gamma= F \cup E_1 \cup\cdots\cup E_s,

where FF is finite, 1≤s≤21 \le s \le2, and each EiE_i is infinite and satisfies

lim⁡N→∞gcd⁡{r∈Ei:r≥N}=∞.\lim_{N \to\infty}\gcd\{r \in E_i : r \ge N\} = \infty.

Next, since 2,3,ℓj2,3,\ell_j are all different from 5, we have 5∤r5 \nmid r for every r∈Γr \in\Gamma. Hence

∣e(r/5)−1∣≥2sin⁡(π/5)>0for any r∈Γ.|e(r/5)-1| \ge2\sin(\pi/5) > 0\qquad\text{for any }r \in\Gamma.

Thus (2) holds with

m=1,α1=15,δ=2sin⁡(π/5).m=1,\qquad\alpha_1=\frac{1}{5},\qquad\delta=2\sin(\pi/5).

Theorem 1.2 now gives the required system and Borel set.

Finally, since 2,3∈Γ2,3 \in\Gamma, we have {2a3b:a,b∈N0}⊂Γ\{2^a3^b : a,b \in\mathbb{N}_0\} \subset\Gamma. Moreover, ℓj∣2jℓj∈Γ\ell_j \mid2^j\ell_j \in\Gamma for any j≥1j \ge1. If Γ\Gamma were generated by finitely many positive integers b1,…,btb_1,\ldots,b_t, every ℓj\ell_j would divide b1⋯btb_1\cdots b_t, which is impossible since the primes ℓj\ell_j are all distinct. Therefore Γ\Gamma 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⊂NQ \subset\mathbb{N} be infinite with 1∈Q1 \in Q. Suppose there exist unit complex numbers ζ\zeta and λk≠1\lambda_k \ne1, k≥1k \ge1, such that

inf⁡r∈Q∣ζr−1∣>0,lim⁡k→∞sup⁡r∈Q∣λkr−1∣=0.\inf_{r \in Q}|\zeta^r-1| > 0,\qquad\lim_{k \to\infty}\sup_{r \in Q}|\lambda_k^r-1|=0.

Then there exist an invertible weakly mixing probability-preserving system (X,B,μ,T)(X,\mathcal{B},\mu,T) and a Borel set A⊂XA \subset X satisfying

μ(A)>0,A∩T−rA=∅(r∈Q).\mu(A)>0,\qquad A\cap T^{-r}A=\varnothing\quad(r\in Q).

Corollary 4.5. Let P={p1,…,pd}\mathcal{P} = \{p_1,\ldots,p_d\} be a finite nonempty set of primes, let h∈Zh \in\mathbb{Z}, and put

SP={p1n1⋯pdnd:n1,…,nd∈N0}.S_{\mathcal{P}} = \{p_1^{n_1}\cdots p_d^{n_d}: n_1,\ldots,n_d \in\mathbb{N}_0\}.

There exist an invertible weakly mixing probability-preserving system (X,B,μ,T)(X,\mathcal{B},\mu,T) and a Borel set A⊂XA \subset X such that

μ(A)>0,A∩T−rA=∅(r∈(SP+h)∩N).\mu(A)>0,\qquad A\cap T^{-r}A=\varnothing\quad(r\in(S_{\mathcal{P}}+h)\cap\mathbb{N}).

The system and the set may depend on hh.

Proof. For h=0h=0, the conclusion follows from Theorem 1.1. Suppose h≠0h\ne0. By Lemma 4.1, write SP=F∪E1∪⋯∪EsS_{\mathcal{P}}=F\cup E_1\cup\cdots\cup E_s, where FF is finite and each EiE_i is infinite and satisfies

lim⁡N→∞gcd⁡{r∈Ei:r≥N}=∞.\lim_{N\to\infty}\gcd\{r\in E_i:r\ge N\}=\infty.

For each 1≤i≤s1\le i\le s, choose integers ci>∣h∣c_i>|h| and Li>∣h∣L_i>|h| such that

ci∣r(r∈Ei, r≥Li).c_i\mid r\qquad(r\in E_i,\ r\ge L_i).

Put Ei′=Ei∩[Li,∞)E_i'=E_i\cap[L_i,\infty). Each Ei′E_i' is infinite and still satisfies the same condition on greatest common divisors. Apply Lemma 3.1 to Ei′E_i' with η=1\eta=1. We obtain Ei′=Ci,0⊔Ci,1E_i'=C_{i,0}\sqcup C_{i,1} and unit complex numbers λi,ϵ,k≠1\lambda_{i,\epsilon,k}\ne1 such that

λi,ϵ,k→1,sup⁡r∈Ci,ϵ∣λi,ϵ,kr−1∣→0\lambda_{i,\epsilon,k}\to1,\qquad\sup_{r\in C_{i,\epsilon}}\left|\lambda_{i,\epsilon,k}^{r}-1\right|\to0

as k→∞k\to\infty, for ϵ=0,1\epsilon=0,1.

Fix ii and ϵ\epsilon, and define Qi,ϵ=(Ci,ϵ+h)∪{1}Q_{i,\epsilon}=(C_{i,\epsilon}+h)\cup\{1\}. Since Li>∣h∣L_i>|h|, all elements of Ci,ϵ+hC_{i,\epsilon}+h are positive. Moreover, Qi,ϵQ_{i,\epsilon} is infinite and contains 11. For every r∈Ci,ϵr\in C_{i,\epsilon},

∣λi,ϵ,kr+h−1∣≤∣λi,ϵ,kr−1∣+∣λi,ϵ,kh−1∣≤∣λi,ϵ,kr−1∣+∣h∣∣λi,ϵ,k−1∣.\begin{aligned} \left|\lambda_{i,\epsilon,k}^{r+h}-1\right|\le\left|\lambda_{i,\epsilon,k}^{r}-1\right|+\left|\lambda_{i,\epsilon,k}^{h}-1\right| \\ &\le\left|\lambda_{i,\epsilon,k}^{r}-1\right|+|h|\left|\lambda_{i,\epsilon,k}-1\right|. \end{aligned}

Consequently,

sup⁡n∈Qi,ϵ∣λi,ϵ,kn−1∣≤sup⁡r∈Ci,ϵ∣λi,ϵ,kr−1∣+(∣h∣+1)∣λi,ϵ,k−1∣⟶0.\sup_{n\in Q_{i,\epsilon}}\left|\lambda_{i,\epsilon,k}^{n}-1\right| \le\sup_{r\in C_{i,\epsilon}}\left|\lambda_{i,\epsilon,k}^{r}-1\right|+(|h|+1)\left|\lambda_{i,\epsilon,k}-1\right|\longrightarrow0.

Next, let ζi=e(1/ci)\zeta_i=e(1/c_i). Since ci∣rc_i\mid r for r∈Ci,ϵr\in C_{i,\epsilon}, ζir+h=e(h/ci)\zeta_i^{r+h}=e(h/c_i). As 0<∣h∣<ci0<|h|<c_i, we have

inf⁡n∈Qi,ϵ∣ζin−1∣≥min⁡{∣e(h/ci)−1∣,∣e(1/ci)−1∣}>0.\inf_{n\in Q_{i,\epsilon}}\left|\zeta_i^n-1\right|\ge\min\{|e(h/c_i)-1|,|e(1/c_i)-1|\}>0.

Thus Qi,ϵQ_{i,\epsilon} 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,ϵQ_{i,\epsilon}.

The remaining positive times belong to the finite set

H=((F∪⋃i=1s(Ei∖Ei′))+h)∩N.H=\left(\left(F\cup\bigcup_{i=1}^{s}(E_i\setminus E_i')\right)+h\right)\cap\mathbb{N}.

If HH is nonempty, apply Lemma 2.4 to HH. Since

(SP+h)∩N⊂H∪⋃i=1s⋃ϵ=01Qi,ϵ,(S_{\mathcal{P}}+h)\cap\mathbb{N}\subset H\cup\bigcup_{i=1}^{s}\bigcup_{\epsilon=0}^{1}Q_{i,\epsilon},

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,R=F\cup E_1\cup\cdots\cup E_s\subset\mathbb{N},

where FF is finite, each EiE_i is infinite, and

lim⁡N→∞gcd⁡{r∈Ei:r≥N}=∞(1≤i≤s).\lim_{N\to\infty}\gcd\{r\in E_i:r\ge N\}=\infty\qquad(1\le i\le s).

Then, for every h∈Z∖{0}h \in\mathbb{Z} \setminus\{0\}, there exist an invertible weakly mixing system (X,B,μ,T)(X,\mathcal{B},\mu,T) and a Borel set AA such that

μ(A)>0,A∩T−rA=∅(r∈(R+h)∩N).\mu(A)>0,\qquad A\cap T^{-r}A=\varnothing\quad(r\in(\mathbb{R}+h)\cap\mathbb{N}).

Indeed, for each ii, we can choose ci>∣h∣c_i>|h| and Li>∣h∣L_i>|h| such that

ci∣r(r∈Ei, r≥Li).c_i\mid r\qquad(r\in E_i,\ r\ge L_i).

Hence

∣e((r+h)/ci)−1∣=∣e(h/ci)−1∣>0.\left|e((r+h)/c_i)-1\right|=\left|e(h/c_i)-1\right|>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 SS of a compact metric space YY is topologically transitive if for any nonempty open sets U,V⊂YU,V\subset Y, some n≥0n\ge0 satisfies U∩S−nV≠∅U\cap S^{-n}V\ne\varnothing. It is topologically weakly mixing if S×SS\times S is topologically transitive on Y×YY\times 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}\mathcal{P}=\{p_1,\ldots,p_d\} be a finite nonempty set of primes, and put

SP={p1n1⋯pdnd:n1,…,nd∈N0}.S_{\mathcal{P}}=\{p_1^{n_1}\cdots p_d^{n_d}:n_1,\ldots,n_d\in\mathbb{N}_0\}.

There exist a compact set Y⊂{0,1}ZY\subset\{0,1\}^{\mathbb{Z}} with S(Y)=YS(Y)=Y for the shift (Sy)n=yn+1(Sy)_n=y_{n+1}, and a nonempty clopen set U⊂YU\subset Y, such that

U∩S−rU=∅(r∈SP).U\cap S^{-r}U=\varnothing\qquad(r\in S_{\mathcal{P}}).

The shift on YY is topologically weakly mixing and admits a full-support weakly mixing invariant Borel probability measure.

Proof. Take (X,B,μ,T)(X,\mathcal{B},\mu,T) and AA from Theorem 1.1. Define

Φ(x)n=1A(Tnx),m=Φ∗μ,Y=supp⁡m.\Phi(x)_n=1_A(T^n x),\qquad m=\Phi_*\mu,\qquad Y=\operatorname{supp}m.

Since Φ∘T=S∘Φ\Phi\circ T=S\circ\Phi and T∗μ=μT_*\mu=\mu, we have S∗m=mS_*m=m and S(Y)=YS(Y)=Y. Moreover, applying (3) to f∘Φf\circ\Phi and g∘Φg\circ\Phi shows that (Y,m,S)(Y,m,S) is weakly mixing. For the clopen set U={y∈Y:y0=1}U=\{y\in Y:y_0=1\},

m(U)=μ(A)>0,m(U)=\mu(A)>0,
m(U∩S−rU)=μ(A∩T−rA)=0(r∈SP).m(U\cap S^{-r}U)=\mu(A\cap T^{-r}A)=0\qquad(r\in S_{\mathcal{P}}).

Each U∩S−rUU\cap S^{-r}U is open in YY, so full support makes it empty. To check topological weak mixing, take nonempty open sets U1,U2,V1,V2⊂YU_1,U_2,V_1,V_2\subset Y. Since mm has full support, we have ci:=m(Ui)m(Vi)>0c_i:=m(U_i)m(V_i)>0. By (3),

1N#{1≤n≤N:m(Ui∩S−nVi)=0}≤1ciN∑n=1N∣m(Ui∩S−nVi)−ci∣⟶0.\frac{1}{N}\#\{1\le n\le N:m(U_i\cap S^{-n}V_i)=0\} \le\frac{1}{c_iN}\sum_{n=1}^{N}|m(U_i\cap S^{-n}V_i)-c_i|\longrightarrow0.

There is therefore a common nn for which both intersections have positive measure. Since open rectangles form a base for Y×YY\times Y, this proves topological transitivity of S×SS\times S. □

The same construction applies to Theorem 1.2, Corollaries 4.3 and 4.5, and Remark 4.6.

Acknowledgments

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

Email address: [email protected]

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