Research article

Exponential sums involving the divisor function over arithmetic progressions

  • Received: 04 November 2022 Revised: 13 February 2023 Accepted: 23 February 2023 Published: 08 March 2023
  • MSC : 11F30, 11L07, 11N37

  • Let ϕ(x) be a smooth function supported on [1,2] with derivatives bounded by ϕ(j)(x)1 and d3(n) be the number of ways to write n as a product of three factors. We get the asymptotic formula for the nonlinear exponential sum n  l mod qd3(n)ϕ(nX)e(33knq).

    Citation: Rui Zhang, Yang Li, Xiaofei Yan. Exponential sums involving the divisor function over arithmetic progressions[J]. AIMS Mathematics, 2023, 8(5): 11084-11094. doi: 10.3934/math.2023561

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  • Let ϕ(x) be a smooth function supported on [1,2] with derivatives bounded by ϕ(j)(x)1 and d3(n) be the number of ways to write n as a product of three factors. We get the asymptotic formula for the nonlinear exponential sum n  l mod qd3(n)ϕ(nX)e(33knq).



    The divisor functions

    dk(n)=n1n2nk=n1

    are the basic arithmetic functions in number theory, and it generate the Dirichlet series ζk(s) which are the simplest GLkL-functions. Hence the behavior of the divisor functions are very important in the theory of automorphic L-funcions. In this article, we will study the sum of the type

    n  l mod qd3(n)ϕ(nX)e(33knq), (1.1)

    where ϕ(x) is a C-function supported on [1,2] with derivatives bounded by ϕ(j)(x)1 and kZ+.

    Studying the asymptotic distribution of this type of sums that involving the Fourier coefficients and the nonlinear exponential functions are very classical in analytic number theory. The oscillation behavior of Fourier coefficients of GL2 automorphic forms is studied by Ren and Ye [13] and they proved an asymptotic formula for the sum

    X<n2Xλf(n)e(αn),

    where λf(n) is the n-th Fourier coefficient of a holomorphic cusp form for GL2. The analytic properties of λf(n) were studied by many authors, see [7,8,9,10,19,20,21,22,23]. For the Maass forms on GL2, Sun and Wu [16] proved the similar asymptotic formula. Acharya and Singh [1] gave the upper bound of the sum

    N<n2Nλf(n)ν(n)e(αnθ),

    where α, θ are real numbers with 0<θ<1, and ν(n) is either μ(n) or Λ(n). If f(x) is a Hecke-Maass cusp form for SL(3,Z), Ren and Ye [14] proved an asymptotic formula for the sum

    n1Af(1;n)ϕ(nX)e(33kn),

    where Af(1;n) is the (1,n)-th Fourier coefficients of f. Let f be a full-level cusp form for GLm(Z) with Fourier coefficients Af(n1,,nm1), Ren and Ye [15] considered the following exponential sums:

    X<|n|2XAf(n,1,,1)e(±α|n|1/m),
    n0Af(n,1,,1)e(±α|n|1/m)ϕ(|n|X).

    They obtained the asymptotic formulas and upper bounds for these sums.

    When the summation is restricted in arithmetic progressions, Yan [18] has proved an asymptotic formula for

    X<n2Xn  l mod qλf(n)e(±2knq),  kZ+,

    where λf(n) is the n-th Fourier coefficient of a holomorphic cusp form for SL(2,Z). Ma and Yan [12] also focused on the oscillation behavior of the exponential sum twisted by r(n) over the arithmetic progressions, where r(n) denote{s} the number of representations of a positive integer n as a sum of two squares. He [3] studied the asymptotic formula for the corresponding GL3 exponential sum

    X<n2Xn  l mod qAf(m;n)ϕ(nX)e(33knq),  kZ+.

    The divisor functions are involving the theory of GLkL-functions. Sun and Zhang [17] studied the average behavior of the divisor functions over values of quadratic forms and got its asymptotic formula. And the general divisor problems involving Hecke eigenvalues also have attracted many authors, see [4,5]. In this paper, we consider the oscillation behavior of the divisor functions dk(n) in arithmetic progressions when k=3. More precisely, the aim of this paper is to prove the following result.

    Theorem 1. Let k,l,qN. Then for any ϵ>0 and qX13ϵ, we have

    n  l mod qd3(n)ϕ(nX)e(33knq)=1q2a mod q(a,q)=1e(alq)0P(logx)ϕ(xX)e(33kxq)dx+3X23q3k13ia mod q(a,q)=1e(alq)(A(k,aq)+B(k,aq))c(ϕ)+O(q52X23+ϵ+q12+ϵk712+ϵX13),

    where A(k,aq) and B(k,aq) are defined in Lemma 2.1 and c(ϕ)=0uϕ(u3)du.

    An interesting generalization of this problem is to replace the exponential function e(33knq) in (1.1) with the q-exponential function eq(z) or the degenerate exponential function etλ for their definitions and properties see Chung-Kim-Kwon [2] and Kim-Kim [11] respectively.

    To prove our theorem, we need the following lemmas.

    Lemma 2.1. Let f(x) be a smooth function of compact support in (0,) and d3(n) be the number of ways to write n as a product of three factors. Then we have

    n=1f(n)d3(n)e(hnk)=1k0P(logx)f(x)dx+π32k3n=1A(n,hk)0U(π3nxk3)f(x)dx+iπ32k3n=1B(n,hk)0V(π3nxk3)f(x)dx, (2.1)

    where

    A(n,hk)=12n1n2n3=nkx1=1kx2=1kx3=1{e(n1x1+n2x2+n3x3+hx1x2x3k)  +e(n1x1+n2x2+n3x3hx1x2x3k)}, (2.2)
    B(n,hk)=12n1n2n3=nkx1=1kx2=1kx3=1{e(n1x1+n2x2+n3x3+hx1x2x3k)  e(n1x1+n2x2+n3x3hx1x2x3k)} (2.3)

    and

    U(x)=12πi13+i13iΓ3(s2)Γ3(1s2)dsxs,     V(x)=12πi13+i13iΓ3(1+s2)Γ3(2s2)dsxs. (2.4)

    Proof. See the Section 5 of Ivić [6].

    Lemma 2.2. If A(n,hk) is defined by (2.2), then for (h,k)=1 we have

    A(n,hk)ϵk32+ϵn14+ϵ.

    Proof. See the Section 8 of Ivić [6].

    Lemma 2.3. If U(x) and V(x) are defined by (2.4), then for any fixed integer K1 and xx0>0

    U(x)=Kj=1cjcos(6x1/3)+djsin(6x1/3)xj/3+O(1x(K+1)/3), (2.5)
    V(x)=Kj=1ejcos(6x1/3)+fjsin(6x1/3)xj/3+O(1x(K+1)/3), (2.6)
    U(x)dx=Kj=0gjcos(6x1/3)+hjsin(6x1/3)x(j1)/3+O(1xK/3), (2.7)
    V(x)dx=Kj=0kjcos(6x1/3)+ljsin(6x1/3)x(j1)/3+O(1xK/3) (2.8)

    with suitable constants cj,,lj, and in particular

    c1=0,   d1=23π,   e1=23π,   f1=0,g0=13π,   h0=0,   k0=0,   l0=13π.

    Proof. See the Lemma 3 of Ivić [6].

    Denote α=33kq. We consider the sum

    S:=S(k,l,q,X)=nl mod qd3(n)ϕ(nX)e(α3n). (3.1)

    Note that

    c|qa mod c(a,c)=1e(anc)={q,q|n;0,otherwise.

    Then

    S=1qc|qa mod c(a,c)=1e(alc)n1d3(n)e(anc)ϕ(nX)e(α3n). (3.2)

    Applying Lemma 2.1 with f(x)=ϕ(x/X)e(α3x), we have

    n1d3(n)e(anc)f(n)=1c0P(logx)f(x)dx+π32c3n1A(n,ac)0U(π3nxc3)f(x)dx+iπ32c3n1B(n,ac)0V(π3nxc3)f(x)dx=:S0(a,c)+S1(a,c)+S2(a,c), (3.3)

    where

    S0(a,c)=1c0P(logx)f(x)dx,S1(a,c)=π32c3n1A(n,ac)ψ1(π3nc),   ψ1(π3nc)=0U(π3nxc3)f(x)dx,S2(a,c)=iπ32c3n1B(n,ac)ψ2(π3nc),   ψ2(π3nc)=0V(π3nxc3)f(x)dx. (3.4)

    Applying Lemma 2.3 with K=3, we obtain

    ψ1(π3nc)=3j=10f(x)cjcos(6π3nxc)+djsin(6π3nxc)πjcj(nx)j/3dx+O(π4c4n43X23+ϵ), (3.5)
    ψ2(π3nc)=3j=10f(x)ejcos(6π3nxc)+fjsin(6π3nxc)πjcj(nx)j/3dx+O(π4c4n43X23+ϵ). (3.6)

    By Lemma 2.2, the O-term in (3.5) contributes to S1(a,c)

    c3n1A(n,ac)π4c4n43X23+ϵc52X23+ϵ.

    By Lemma 2.2, the O-term in (3.6) contributes to S2(a,c)

    c3n1B(n,ac)π4c4n43X23+ϵc52X23+ϵ.

    For the integral in (3.5) and (3.6), we make a change of variable x=Xu3 to get

    0ϕ(xX)e(α3x±33nxc)cj(π3nx)j/3dx=3X0ϕ(u3)e((α±33nc)3Xu)cjπj(nX)j/3uju2du=3Xcj(π3nX)j/3I±j(nc3), (3.7)

    where

    I±j(nc3)=321u2jϕ(u3)e((α±33nc)3Xu)du. (3.8)

    By (3.4)–(3.7), we have

    S1(a,c)=3π32c3n1A(n,ac)3j=1Xcj(π3nX)j/3(cj2I+j(nc3)+cj2Ij(nc3)     +dj2iI+j(nc3)dj2iIj(nc3))+O(c52X23+ϵ),
    S2(a,c)=i3π32c3n1B(n,ac)3j=1Xcj(π3nX)j/3(ej2I+j(nc3)+ej2Ij(nc3)     +fj2iI+j(nc3)fj2iIj(nc3))+O(c52X23+ϵ).

    Let

    F±(u):=F±(u,n)=(α±33nc)3Xu.

    Note that

    α3X=33kXq>Xϵ

    for q<X13ϵ. Then

    F+(u)=(α+33nc)3Xα3XXϵ

    and by integration by parts many times, we show that I+j(nc3) is negligible. For n2c3α327 or nc3α3100, we also have

    F(u)=(α33nc)3Xα3XXϵ,

    thus, Ij(nc3) is negligible for n2c3α327 or nc3α3100. Denote

    I=(c3α3100,2c3α327).

    Then we can get

    S1(a,c)=3π322c3nIA(n,ac)3j=1cjπjnj3X1j3(cjIj(nc3)+idjIj(nc3))+O(c52X23+ϵ), (3.9)
    S2(a,c)=i3π322c3nIB(n,ac)3j=1cjπjnj3X1j3(ejIj(nc3)+ifjIj(nc3))+O(c52X23+ϵ). (3.10)

    For j2, we use the trivial bound Ij(nc3)1. Then the contribution from Ij(nc3), j=2,3 to S1(a,c) in (3.9) and S2(a,c) in (3.10) is at most

    c94+ϵα74X13.

    Then, by Lemma 2.3, (3.9) and (3.10), we have

    S1(a,c)=3c2iX23nIA(n,ac)n13I1(nc3)+O(c52X23+ϵ+c94+ϵα74X13), (3.11)
    S2(a,c)=3c2iX23nIB(n,ac)n13I1(nc3)+O(c52X23+ϵ+c94+ϵα74X13). (3.12)

    Thus, by (3.11) and (3.12), we can get

    S1(a,c)+S2(a,c)=3c2iX23nI(A(n,ac)+B(n,ac))n13I1(nc3)+O(c52X23+ϵ+c94+ϵα74X13). (3.13)

    Note that the first term in (3.13) disappears when α332c. For α>332c, let nα1 be the integer such that

    (cα3)3=nα+λ,     12<λ12. (3.14)

    Then for any positive integer n, we have

    |33ncα|=3c|3ncα3|=3|nnαλ|c(3n2+3n(cα3)+(cα3)2).

    For nnα, the right-hand side of above equation

    |nnα|c3α2,

    and then

    F(u,n)|nnα|c3α23X.

    By integrating by parts, we can obtain

    I1(nc3)c3α23X|nnα|.

    Thus, by Lemma 2.2, the contribution of the term nnα to (3.13) is at most

    c2X23c3α2X13nI{nα}(A(n,ac)+B(n,ac))n13|nnα|1c1+ϵα2X13nI{nα}c32+ϵn1413+ϵ|nnα|1c94+ϵα74+ϵX13nI{nα}|nnα|1c94+ϵα74+ϵX13.

    When n=nα, we can get

    |F(u,n)|c3α2X13|λ|.

    For |λ|110, we have I1(nαc3)c3α2X13 by integrating by parts. Hence, the first term in (3.13) is bounded by c94+ϵα74+ϵX13. If c3α2X13|λ|Xϵ, then I1(nαc3) is negligible. This proves that

    S1(a,c)+S2(a,c)=ϑα3ic23nα3X2(A(nα,ac)+B(nα,ac))I1(nαc3)+O(c52X23+ϵ+c94+ϵα74X13), (3.15)

    where

    ϑα={1,    nαI, s.t.|nα2c3α327|<min{c3α2X13+ϵ,110};0,   otherwise.

    By (3.2), (3.3) and (3.15), we have

    S=ϑα3iq3nα3X2c|q1c2a mod c(a,c)=1e(alc)(A(nα,ac)+B(nα,ac))I1(nαc3)+1qc|qa mod c(a,c)=1e(alc)S0(a,c)+O(q52X23+ϵ+q94+ϵα74X13).

    Since α=33kq with kZ, we have cq. Then

    |kkc3q3|=kc3q3|c3q31|kc3q3c3α2X13+ϵ.

    Thus, kc3q3=0 for cq. Otherwise, we take

    c=q,   nα=k.

    Therefore,

    S=3iq33k3X2a mod q(a,q)=1e(alq)(A(k,aq)+B(k,aq))c(ϕ)+1qa mod q(a,q)=1e(alq)S0(a,q)+O(q52X23+ϵ+q12+ϵk712+ϵX13), (3.16)

    where

    c(ϕ)=0uϕ(u3)du

    and

    S0(a,q)=1q0P(logx)ϕ(xX)e(33kxq)dx.

    This proves our theorem.

    This paper focused on the study of the nonlinear exponential sum twisting the divisor functions d3(n) over the arithmetic progression and established its asymptotic formula. The main techniques used to prove the theorem were the estimation of exponential sum, Voronoi summation formula, and the weighted stationary phase. Moreover, it is also an interesting question to generalize the resonance theory to the divisor functions dk(n) if there is a better Voronoi summation formula for k>3, and we can try to obtain a better bound for the error term respect to q which is a prime number.

    Zhang, Li and Yan are supported by the National Natural Science Foundation of China [Grant No. 12171286].

    The authors declare no conflict of interest.



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