The article considers a generalization of Piatetski-Shapiro sequences in the sense of Beatty sequences. The sequence is defined by (⌊αnc+β⌋)∞n=1, where α≥1, c>1, and β are real numbers.
The focus of the study is on solving equations of the form ⌊αnc+β⌋=smk, where m and n are positive integers, 1≤n≤N, and s is an integer. Bounds for the solutions are obtained for different values of the exponent k, and an average bound is derived over k-free numbers s in a given interval.
Citation: Yukai Shen. kth powers in a generalization of Piatetski-Shapiro sequences[J]. AIMS Mathematics, 2023, 8(9): 22411-22418. doi: 10.3934/math.20231143
[1] | Zhao Xiaoqing, Yi Yuan . Square-free numbers in the intersection of Lehmer set and Piatetski-Shapiro sequence. AIMS Mathematics, 2024, 9(12): 33591-33609. doi: 10.3934/math.20241603 |
[2] | Victor Zhenyu Guo . Almost primes in Piatetski-Shapiro sequences. AIMS Mathematics, 2021, 6(9): 9536-9546. doi: 10.3934/math.2021554 |
[3] | Jinyun Qi, Zhefeng Xu . Almost primes in generalized Piatetski-Shapiro sequences. AIMS Mathematics, 2022, 7(8): 14154-14162. doi: 10.3934/math.2022780 |
[4] | Xiaoge Liu, Yuanyuan Meng . On the $ k $-th power mean of one kind generalized cubic Gauss sums. AIMS Mathematics, 2023, 8(9): 21463-21471. doi: 10.3934/math.20231093 |
[5] | Xiaoxue Li, Wenpeng Zhang . A note on the hybrid power mean involving the cubic Gauss sums and Kloosterman sums. AIMS Mathematics, 2022, 7(9): 16102-16111. doi: 10.3934/math.2022881 |
[6] | Tingting Wen . On the number of integers which form perfect powers in the way of $ x(y_1^2+y_2^2+y_3^2+y_4^2) = z^k $. AIMS Mathematics, 2024, 9(4): 8732-8748. doi: 10.3934/math.2024423 |
[7] | Guangwei Hu, Huixue Lao, Huimin Pan . High power sums of Fourier coefficients of holomorphic cusp forms and their applications. AIMS Mathematics, 2024, 9(9): 25166-25183. doi: 10.3934/math.20241227 |
[8] | Li Zhou, Liqun Hu . Sum of the triple divisor function of mixed powers. AIMS Mathematics, 2022, 7(7): 12885-12896. doi: 10.3934/math.2022713 |
[9] | Zhenjiang Pan, Zhengang Wu . The inverses of tails of the generalized Riemann zeta function within the range of integers. AIMS Mathematics, 2023, 8(12): 28558-28568. doi: 10.3934/math.20231461 |
[10] | Huimin Wang, Liqun Hu . Sums of the higher divisor function of diagonal homogeneous forms in short intervals. AIMS Mathematics, 2023, 8(10): 22577-22592. doi: 10.3934/math.20231150 |
The article considers a generalization of Piatetski-Shapiro sequences in the sense of Beatty sequences. The sequence is defined by (⌊αnc+β⌋)∞n=1, where α≥1, c>1, and β are real numbers.
The focus of the study is on solving equations of the form ⌊αnc+β⌋=smk, where m and n are positive integers, 1≤n≤N, and s is an integer. Bounds for the solutions are obtained for different values of the exponent k, and an average bound is derived over k-free numbers s in a given interval.
The Piatetski-Shapiro sequences are defined by N(c)=(⌊nc⌋)∞n=1, where c>1 and c∉N. In 1953, Piatetski-Shapiro [8] proved that N(c) contains infinitely many primes if c∈(1,1211). Moreover, he showed that the prime counting function π(c)(x), which counts the number of primes in N(c) up to x, satisfies the asymptotic relation π(c)(x)∼x1/clogx as x→∞. Since then, the range of c for which it is known that N(c) contains infinitely many primes has been extended several times, and it is now known that the above formula holds for all c∈(1,28172426) thanks to the work of Rivat and Sargos [10].
This study is related to the topic of Beatty sequences. A non-homogeneous Beatty sequence is a sequence of integers obtained from fixed real numbers α>0 and β, defined as Bα,β=(⌊αn+β⌋)∞n=1, which is sometimes referred to a generalized arithmetic progression. It is well-known that the sequence contains infinitely many prime numbers if α is irrational [4]. Moreover, it is possible to establish an asymptotic relation for the distribution of primes in such sequences, which is the subject of extensive research in number theory. We get that
#{prime p≤x:p∈Bα,β}∼α−1π(x),x→∞ |
holds, where π(x) is the prime counting function.
The author of this study proposes a generalization of Piatetski-Shapiro sequences in the context of Beatty sequences, which similarly consists of infinitely many prime numbers. Specifically, let α≥1 and β be real numbers. We investigate the following generalized Piatetski-Shapiro sequences:
N(c)α,β=(⌊αnc+β⌋)∞n=1. |
The Piatetski-Shapiro sequences have deep connections to several fundamental concepts in number theory, such as smooth numbers, square-free numbers and so on. Previous research by Liu, Shparlinski, and Zhang [5] focused on the distribution of squares in Piatetski-Shapiro sequences, while Qi, Guo, and Xu [9] investigated an intriguing equation related to these sequences. In this paper, we aim to extend their work by exploring the distribution of k-th powers in a generalization of Piatetski-Shapiro sequences, which can be viewed as an extension of their previous findings. To be precise, we define Qα,βc,k(s;N) as the number of solutions to the equation:
⌊αnc+β⌋=smk,1≤n≤N,m,n∈Z. |
We mention the trivial bound
Qα,βc,k(s;N)≤min(N,s−1k(αNc+β)1k). |
We prove the following theorem.
Theorem 1.1. Let k>1 be an integer. For any exponent pair (κ,λ), we have
Qα,βc,k(s;N)=γ(kγ−k+1)−1s−1kN1−c+ck+O(s−λk(1+κ)Nkκ+cλk(1+κ)+ε+sκ−λkNkκ+c(λ−κ)k+ε+s−1kN−c+ck). |
We also study Qα,βc,k(s;N) on average over positive k-free integers s≤S. Recall that γ=c−1and define that
Qα,βc,k(S,N)=∑s≤Ss is k-free Qα,βc,k(s;N). |
We remark that only the case S≤αNc+β is meaningful, hence we always assume this. Liu, Shparlinski and Zhang [5] showed that
Q1,0c,2(S,N)=12γπ2(2γ−1)S1−1kN1−c2+O(S15N15+2c5+S58N3c8+S18N14+3c8+SN1−c). |
We obtain the following result.
Theorem 1.2. For any c>1,c∉N, we have
Qα,βc,k(S,N)=kζ(k)(k−1)(kγ−k+1)S1−1kN1−c+ck+O(S35−45kN15+4c5k+S1−34kN3c4k+S12−34kN14+3c4k+SN1−c+S1−1kN−c+ck). |
We remark that the topic is relative to harmonic numbers and their relationships which are interesting mathematical concepts, including number theory, calculus, and physics, as well as the study of degenerate versions or special cases.For further details, refer to [6,7].
We denote by ⌊t⌋ and {t} the greatest integer ⩽t and the fractional part of t, respectively. We also write e(t)=e2πit for all t∈R, as usual. We make considerable use of the sawtooth function defined by
ψ(t)=t−⌊t⌋−12={t}−12(t∈R). |
In this study, we consider the Piatetski-Shapiro sequence (⌊nc⌋)∞n=1, where ⌊⋅⌋ denotes the floor function, and γ is defined as the inverse of the constant c. The set of primes in the natural numbers is denoted by P. We use the notation m∼M to indicate that m lies in the interval (M,2M].
In order to state our results, we introduce some notation. Throughout the paper, the symbol ε represents an arbitrarily small positive constant, which may vary from one occurrence to another. The implied constants in the symbols O, ≪, and ≫ may depend on the parameters c, ε, α, and β, but are absolute otherwise. For given functions F and G, the notations F≪G, G≫F, and F=O(G) are all equivalent to the assertion that the inequality |F|⩽C|G| holds with some constant C>0.
Lemma 2.1. Let
L(Q)=I∑i=1AiQai+J∑j=1BjQ−bj, |
where Ai,ai,Bj,bj>0. Then, (1) for any Q2≥Q1>0 there exists Q∈[Q1,Q2] such that
L(Q)≪I∑i=1J∑j=1(AbjiBaij)1ai+bj+I∑i=1AiQai1+J∑j=1BjQ−bj2. |
(2) For any Q1>0 there exists Q∈(0,Q1] such that
L(Q)≪I∑i=1J∑j=1(AbjiBaij)1ai+bj+J∑j=1BjQ−bj1. |
Proof. See [3, Lemma 2.4]
Lemma 2.2. For any J>0, there holds
ψ(x)=∑1≤|j|≤Jaje(jx)+O(∑|j|≤Jbje(jx)), |
where
aj≪|j|−1,bj≪J−1. |
Proof. This is the result of Vaaler [11].
Lemma 2.3. (1384+ε,5584+ε) is an exponent pair.
Proof. See [1, Theorem 6].
Lemma 2.4. Let α,α1,α2 be real constants such that
α∉1andαα1α2∉0. |
Let M,M1,M2,x≥1 and let
Φ=(φm)m∼MandΨ=(ψm1,m2)m1∼M1,m2∼M2 |
be two sequences of complex numbers supported on m∼M,m1∼M1 and m2∼M2 with |φm|≤1. Then, for the sum
SΦ,Ψ(x;M,M1,M2)=∑m∼M∑m1∼M1∑m2∼M2φmψm1,m2e(xmαmα11mα22MαMα11Mα22) |
we have
SΦ,Ψ(x;M,M1,M2)≪(x14M12(M1M2)34+M710M1M2+M(M1M2)34+x−14M1110M1M2)log2(2MM1M2). |
Proof. See [2, Theorem 3]
Denote γ=c−1 and θ=α−γ. A kth power equals ⌊αnc+β⌋ if and only if
smk≤αnc+β<smk+1, |
which is equivalent to
θ(smk−β)γ≤n<θ(smk+1−β)γ. |
Let M=s−1k(αNc+β)1k, by a normal construction,
Qα,βc,k(s;N)=∑m≤M(⌊−θ(smk−β)γ⌋−⌊−θ(smk+1−β)γ⌋)+O(1)=S1+S2+O(1), | (3.1) |
where
S1=∑m≤M(θ(smk+1−β)γ−θ(smk−β)γ)=θ∑m≤M(γ(smk−β)γ−1+O((smk−β)γ−2))=θ∑m≤M(γsγ−1mk(γ−1)+O(sγ−2mk(γ−2)))=γ(kγ−k+1)−1s−1kN1−c+ck+O(s−1kN−c+ck), | (3.2) |
and
S2=∑m≤M({−θ(smk+1−β)γ}−{−θ(smk−β)γ})=∑m≤M(ψ(−θ(smk+1−β)γ)−ψ(−θ(smk−β)γ)). |
Consider S2. From Lemma 2.2 we have
S2=S3+O(S4), | (3.3) |
where
S3=∑m≤M∑1≤|j|≤Jaj(e(−jθ(smk+1−β)γ)−e(−jθ(smk−β)γ)), |
and
S4=∑m≤M∑|j|≤Jbj(e(−jθ(smk+1−β)γ)+e(−jθ(smk−β)γ)), |
for any J≥1. We begin with S3. Remembering aj≪|j|−1, we have
S3≪∑1≤|j|≤J|j|−1|∑m≤Me(jθsγmkγ)|. |
Summing over m, we obtain
∑m≤Me(jθsγmkγ)≪logMmax1≤L≤M|∑L≤m≤2Le(jθsγmkγ)|. |
Using the exponent pair (κ,λ) we get
∑L≤m≤2Le(jθsγmkγ)≪(jθsγLkγ−1)κLλ. |
Then,
∑m≤Me(jθsγmkγ)≪jκθκsκ−λkNc(kγκ−κ+λ)k+ε, |
which yields
S3≪Jκθκsκ−λkNc(kγκ−κ+λ)k+ε. |
We can readily eliminate the contribution of S4. By utilizing the fact that bj is bounded by J−1, we obtain the following result:
S4≪J−1∑|j|≤J|∑m≤Me(jθsγmkγ)|≪J−1s−1kNck+J−1∑1≤|j|≤J|∑m≤Me(jθsγmkγ)|. |
By a similar argument, we have
S4≪J−1s−1kNck+Jκsκ−λkNc(kγκ−κ+λ)k+ε. |
It yields that
J=sλ−κ−1k+kκNc(1+κ−kγκ−λ)k+kκ. |
Applying Lemma 2.1 to the bounds on terms in (3.3), we have
S2≪s−λk(1+κ)Nkκ+cλk(1+κ)+ε+sκ−λkNkκ+c(λ−κ)k+ε. |
Now the result follows from (3.3) and (3.1). Applying the exponent pair (1384+ε,5584+ε) from Lemma 2.3 by Bourgain [1], people can get the asymptotic formula
Qα,βc,k(s;N)=γ(kγ−k+1)−1s−1kN1−c+ck+O(s−5597kN1397+55c97k+ε+s−12kN1384+c2k+ε). |
This proof is almost identical to the proof given in [5, Theorem 2.3], so we will provide only a brief outline. We start that
Φk(S)=∑s≤Ss is k-free s−1k. |
Applying a commonly known result, (see [11, p. 181]),
∑s≤Ss is k-free 1=Sζ(k)+O(S1k), |
and a partial summation, we obtain
Φk(S)=kζ(k)(k−1)S1−1k+O(logS). | (4.1) |
We proceed as in the proof of Theorem 1.1, so set θ=α−γ, T=(αNc+β)γ, and
Qα,βc,k(S;N)=K0+K1+O(1), |
where
K0=∑smk≤αNc+βs≤Ss is k-free (θ(smk+1−β)γ−θ(smk−β)γ), |
and
K1=∑smk≤αNc+βs≤Ss is k-free (ψ(−θ(smk+1−β)γ)−ψ(−θ(smk−β)γ)). |
Using (3.2) and (4.1), we compute K0 directly as follows
K0=γ(kγ−k+1)−1N1−c+ckΦk(S)+O(SN1−c+S1−1kN−c+ck). |
By Lemma 2.2
K1≪K11+K12, |
where
K11=∑smk≤αNc+βs≤Ss is k-free ∑0<|j|<Jaj(ψ(−θ(smk+1−β)γ)−ψ(−θ(smk−β)γ)), |
and
K12=∑smk≤αNc+βs≤Ss is k-free ∑0≤|j|<Jbj(ψ(−θ(smk+1−β)γ)−ψ(−θ(smk−β)γ)). |
Using a similar approach in [5, p. 250] we have
K11≪∑0<|j|<Jj−1|S(R,D,M;j)|, |
where
S(R,D,M;j)=∑r∼R,d∼D,m∼Mrdkmk≤αNc+β,rdk≤Sμ(d)e(−jθrγdkγmkγ). |
From Lemma 2.4, we have
S(R,D,M;j)=(jRγDkγMkγ)14R12(DM)34+R710DM+R(DM)34+(jRγDkγMkγ)−14R1110DM. |
Noting that γ>12, it can be easily verified that the fourth term can be combined with the third term on the right-hand side. We can obtain
K11≪j14N14+3c4kS12−34k+NckS710−1k+N3c4kS1−34k. |
Hence,
|K11|+|K12|≪J14N14+3c4kS12−34k+J−1NckS1−1k+NckS710−1k+N3c4kS1−34k, |
where the term J−1NckS1−1k results from the choice j=0 in the summation on the right-hand side in Lemma 2.2. Now Lemma 2.1 gives
|K11|+|K12|≪N15+4c5kS35−45k+N3c4kS1−34k+N14+3c4kS12−34k. |
We have the final result.
We have proved Theorems 1.1 and 1.2.
The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.
The author is supported in part by the Fundamental Research Funds for the Central Universities (No. xzy012021030) and the Shaanxi Fundamental Science Research Project for Mathematics and Physics (No. 22JSY006).
We declare no conflict of interest.
[1] | J. Bourgain, Decoupling, exponential sums and the Riemann zeta function, J. Amer. Math. Soc., 30 (2017), 205–224. |
[2] | E. Fouvry, H. Iwaniec, Exponential sums with monomials, J. Number Theory, 33 (1989), 311–333. |
[3] | S. W. Graham, G. Kolesnik, Van der Corput's Method of Exponential Sums, Cambridge: Cambridge University Press, 1991. |
[4] |
V. Z. Guo, J. Qi, A generalization of Piatetski-Shapiro sequences, Taiwanese J. Math., 26 (2022), 33–47. https://doi.org/10.11650/tjm/210802 doi: 10.11650/tjm/210802
![]() |
[5] | K. Liu, I. E. Shparlinski, T. Zhang, Squares in Piatetski-Shapiro sequences, Acta Arith., 181 (2017), 239–252. |
[6] |
T. Kim, D. S. Kim, Combinatorial identities involving degenerate harmonic and hyperharmonic numbers, Adv. in Appl. Math., 148 (2023), 102535. https://doi.org/10.1016/j.aam.2023.102535 doi: 10.1016/j.aam.2023.102535
![]() |
[7] |
T. Kim, D. S. Kim, Some identities involving degenerate Stirling numbers associated with several degenerate polynomials and numbers, Russ. J. Math. Phys., 30 (2023), 62–75. https://doi.org/10.1134/S1061920823010041 doi: 10.1134/S1061920823010041
![]() |
[8] | I. I. Piatetski-Shapiro, On the distribution of prime numbers in the sequence of the form ⌊f(n)⌋, Mat. Sb., 33 (1953), 559–566. |
[9] |
J. Qi, V. Z. Guo, Z. Xu, kth powers in Piatetski-Shapiro sequences, Int. J. Number Theory, 18 (2022), 1791–1806. https://doi.org/10.1142/S1793042122500919 doi: 10.1142/S1793042122500919
![]() |
[10] | J. Rivat, S. Sargos, Nombres premiers de la forme ⌊nc⌋, Canad. J. Math., 53 (2001), 414–433. |
[11] | J. D. Vaaler, Some extremal problems in Fourier analysis, Bull. Amer. Math. Soc., 12 (1985), 183–216. |