Research article

Sums of the higher divisor function of diagonal homogeneous forms in short intervals

  • Received: 04 June 2023 Revised: 30 June 2023 Accepted: 05 July 2023 Published: 17 July 2023
  • MSC : 11E25, 11N37, 11P55

  • Let dk(n) denote the k-th divisor function. In this paper, we give the asymptotic formula of the sum

    xynrix+yi=1,2,,ldk(nr1+nr2++nrl),

    where n1,n2,,nlZ+, k2, r3 and l>2r1 are integers.

    Citation: Huimin Wang, Liqun Hu. Sums of the higher divisor function of diagonal homogeneous forms in short intervals[J]. AIMS Mathematics, 2023, 8(10): 22577-22592. doi: 10.3934/math.20231150

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  • Let dk(n) denote the k-th divisor function. In this paper, we give the asymptotic formula of the sum

    xynrix+yi=1,2,,ldk(nr1+nr2++nrl),

    where n1,n2,,nlZ+, k2, r3 and l>2r1 are integers.



    For any integer k2, let

    dk(n)=m1m2mk=nm1,m2,,mkZ+1

    define the k-th divisor function and d(n)=d2(n).

    Recently, the sums of divisor function about the quadratic form n21+n22++n2l with l3 has drawn researchers' attention. For k=2 and l=3, in 2000, Calderˊon and de Velasco [1] gave the following asymptotic formula,

    1n1,n2,n3x12d(n21+n22+n23)=4ζ(3)5ζ(4)x32logx+O(x32).

    Later, Guo and Zhai [4] used the classical circle method to solve the case of k=2 and l=3. Furthermore, the error term was eventually upgraded by Zhao [14] to xlog7x. For k=2 and l3, Zhang [15] proved that

    1n1,,nlx12d(n21++n2l)=c1xl2logx+c2xl2+O(xl+14logl+4x+xl22logx),

    where c1 and c2 are constants. Moreover, Lü and Mu [10] considered the nonhomogeneous case, the leading term of

    1n1,n2x121n3x1kd(n21+n22+nk3)

    is x1+1k(1+logx).

    In 2016, Sun and Zhang [12] began to take up the higher divisor function. For k=3 and l=3, they proved that

    1n1,n2,n3x12d3(n21+n22+n23)=c3x32log2x+c4x32logx+c5x32+O(x3218+ε),

    where c3, c4 and c5 are constants. Later, Hu and Yang [8] considered the cases of l=4. For k4 and l3, Hu and Lü [5] investigated that the main term of the sum

    1n1,n2,,nlx12dk(n21+n22++n2l)

    is xl2logk1x.

    Recently, the above results were summarized by Zhou and Ding [17], for r2, k2 and l>2r1,

    1n1,n2,,nlx1rdk(nr1+nr2++nrl)c6xlrlogk1x,

    where c6 is a constant.

    Inspired by the above research involving the divisor function, Hu and Yao [7] considered the sums of divisor of the ternary quadratic form in short intervals. It is stated that, for θ=12+2ε and y=xθ, there holds

    xy<m1,m2,m3x+yd(m21+m22+m23)=c7L1(x,y)+c8L2(x,y)+O(y3ε),

    where c7 and c8 are constants, and Lj(x,y) (j=1,2) satisfies L1(x,y)y3logy, L2(x,y)y3.

    Later, Hu and Liu [6] explored the case of a quaternary quadratic form in short intervals. Moreover, Zhang and Li [16] studied the nonhomogenous case in short intervals. They proved that, y=x1δk+4ε with δ3=215, δk=1k(2k2+1) for 4k7 and δk=1k(k2k+1) for k8, there holds

    xy<mk3x+yxy<m2ix+yi=1,2d(m21+m22+mk3)=c9L1(x,y)+c10L2(x,y)+O(y3x2+1kε),

    where c9 and c10 are constants, and Lj(x,y) (j=1,2) satisfies L1(x,y)y3x2+1klogx, L2(x,y)y3x2+1k.

    In this paper, we will extend the result of Zhou and Ding [17] in short intervals. We want to consider the asymptotic formula of the sum

    Sk(x,y)=xynrix+yi=1,2,,ldk(nr1+nr2++nrl),

    where y=xθ with 0<θ1.

    To give our result, let

    Sr(q,a)=qh=1e(ahrq). (1.1)

    For 0jk1, we define

    Aj(q)=qb=1e(abq)cj+1(b,q), (1.2)

    where a>0 is a positive integer. We learn from [3, p.372] that for (a,q)=1, Aj(q) is independent of a. The coefficients cj(b,q) can be written as

    b1b2b(mod q)f(b1)

    for some function f.

    Meanwhile, the number of terms in cj(b,q) depends only on k. More accurately, the coefficients cj(b,q) are given explicitly in [2, (2.13)]. Also, from [3, (4.8)] we can get

    Aj(q)kq1. (1.3)

    Our result is as follows.

    Theorem 1.1. Let k2, r3 and l>2r1 be integers. We have

    Sk(x,y)=q=11aq(a,q)=1Slr(q,a)qlk1j=0Aj(q)1j!S(x,y)+O(ylxl+lrε),

    where

    θ={(11r)(r2+l2r1k2r1ε)r2+l2r1k2r112εif3r7,(11r)(r2+l2r(r1)k2r(r1)ε)r2+l2r(r1)k2r(r1)12εifr8,

    and Sr(q,a), Aj(q) are defined in (1.1) and (1.2), respectively. Moreover, S(x,y) is defined as

    S(x,y)=1rlxynix+yi=1,2l1(n1ni)11rl(xy)nl(x+y)n1+n2++nl=nlogjn (1.4)

    satisfying S(x,y)ylxl+lrlogjx.

    For this problem, unlike other results, we are interested in how to find a smaller suitable value of θ to make sure that Sk(x,y) has an asymptotic formula. We will establish Theorem 1.1 by the circle method and employ the estimate of the sum of the divisors over the arithmetic progression and some estimates of exponential sum in short intervals.

    Notation: Throughout this paper, x always denotes a sufficiently large positive integer and y=xθ with 0<θ1, we take N1=xy and N2=x+y, f(x)g(x) means that f(x)=O(g(x)), f(x)g(x) means that f(x)g(x)f(x). As usual, ||α|| denotes the distance from α to the nearest integer, e(x)=e2πix, ε always denotes an arbitrary small positive constant, which may not be the same at different occurrences. For λR, we set

    Tr(N1r1,N1r2)=1rN1nN2n1r1e(nλ),
    T(lN1,lN2)=lN1nlN2(logjn)e(nλ).

    We define

    fr(α)=N1r1nN1r2e(αnr), g(α)=lN1nlN2dk(n)e(nα). (1.5)

    We list the following lemmas that will be used in subsequent sections.

    Lemma 2.1. For any real numbers α and τ1, and integers a and q satisfying (a,q)=1,1qτ, α can be written as

    α=aq+λ,|λ|1qτ.

    Proof. See Pan and Pan [11, Lemma 5.19].

    Lemma 2.2. For any a,qZ with 1aq, (a,q)=1.

    Sr(q,a)=qh=1e(ahrq)q11r.

    Proof. See Vaughan [13, Theorem 4.2].

    Lemma 2.3. Let r3 and N1,N2 be defined as above. Then we get

    Tr(N1r1,N1r2)min(yx1+1r,1x11r||λ||), (2.1)
    T(lN1,lN2)logj(lN2)min(y,1||λ||), (2.2)
    T(lN1,lN2)=lN2lN1e(λu)(logju)du+O(logr(lN2)(1+y|λ|)). (2.3)

    Proof. For (2.1), (2.2) and (2.3), see [16, Lemmas 2.5 and 2.9].

    Lemma 2.4. For r 3, We have

    fr(α)=Sr(q,a)qTr(N1r1,N1r2)+O(q11r(1+|λ|y)).

    Proof. See [16, Lemma 2.10].

    Lemma 2.5. Let g(α) be defined in (1.5). Then there holds

    10|g(α)|2dαylogk21x.

    Proof. By the definition of g(α), we have

    10|g(α)|2dα=lN1n1lN2lN1n2lN2dk(n1)dk(n2)10e((n1n2)α)dα=nlN2d2k(n)nlN1d2k(n).

    It follows from [9, Theorem 1] that,

    nxd2k(n)=x(logk21x+logk22x++logx)+O(exp(ec11k2)x1c12k43+ε),

    where k=o(loglogx) and c11,c12>0 are constants. Then we have

    10|g(α)|2dα=lN2logk21(lN2)lN1logk21(lN1)++lN2log(lN2)lN1log(lN1)+O(exp(ec11k2)N1c12k43+ε2).

    Noting the fact that log(1+u)u for u0, we can deduce that

    lN2logk21(lN2)lN1logk21(lN1)=(lN2lN1)logk21(lN2)+lN1(logk21(lN2)logk21(lN1))ylogk21x+N1log(N2N1)logk22xylogk21x+N1log(1+N2N1N1)logk22xylogk21x.

    Therefore, by similar arguments, it's not hard to derive that

    10|g(α)|2dαylogk21x.

    Lemma 2.6. For r2 and fr(α) defined in (1.5), we have

    10|fr(α)|2rdα(yx1+1r)2rr+ε.

    Proof. The proof is similar to that of [13, Lemma 2.5]. We notice that the key of proof of [13, Lemma 2.5] depends on the summation interval. It is showed that the only difference between these two proofs is the length of interval and easily to get N1r2N1r1=(x+y)1r(xy)1ryx1+1r. This completes the proof of Lemma 2.6.

    Lemma 2.7. Suppose that (a,q)=1, qQy1k. We have

    g(α)=k1j=0Aj(q)Ij(λ)+O(Qk+ε+yη+εQ),

    where η=k1k+1 for 2k3, η=k1k+2 for k4, and Aj(q) is defined as in (1.2).

    Proof. When 2k3, by the definition of (1.5), we write

    g(α)=lN1nlN2dk(n)e(αn)=qb=1e(abq)lN1nlN2nb( mod q)dk(n)e(nλ)=qb=1e(abq)lN2lN1e(λu)d(Dk(u;b,q)),

    where

    Dk(u;b,q)=1nunb( mod q)dk(n).

    According to the divisor problem for arithmetic progressions, we utilize it to isolate the main term and estimate the remainder. For the sake of simplicity, we denote

    Dk(u;b,q)=Mk(u;b,q)+k(u;b,q).

    We learn from [2, Theorem 1] that main term has the form

    Mk(u;b,q)=k1j=0cj+1(b,q)Lj(u),

    where Lj(u) is an antiderivative of logju/j!. Thus, the contribution of main term to g(α) can be written as

    g(α)=k1j=0Aj(q)Ij(λ),

    where Aj(q) is defined as in (1.2), and Ij(λ) is defined as in (2.4). After integrating by parts, one has

    Ij(λ)=lN2lN1e(λu)logjuj!duyεmin(y,λ1). (2.4)

    It follows from [3, (4.4)] that the contribution from error term is bounded by

    O(Qk+ε+yη+εQ),

    when k4, the proof is similar, so we omit it.

    In order to apply the circle method, we set

    xεQ<τ, Qτyx11r, Q=y1kx1kr1k. (3.1)

    By Lemma 2.1, each αI:=[1τ,1+1τ) can be written as

    α=aq+λ,|λ|1qτ

    for two positive integers a,q with 1aqτ and (a,q)=1.

    We define the major arcs M and m as follows:

    M=qQ1aq(a,q)=1M(q,a),m=IM,

    where M(q,a)={α:α=aq+λ,|λ|1qτ}.

    It is obvious that the major arcs M are actually disjoint when 1<Q<τ2. Noting that fr(α) and g(α) are defined in (1.5), we obtain

    Sk(x,y)=1+1τ1τflr(α)g(α)dα=Mflr(α)g(α)dα+mflr(α)g(α)dα.

    First, we deal with the integrals over the minor arcs.

    Lemma 3.1. Suppose αm with Q<qτ.

    For 3r7, we have

    mflr(α)g(α)dαylr2+12x(1r1)(lr2)+ε(Q2r1l2r1+y2r1l2r1x(1r1)(2r1l2r1)).

    For r8, we have

    mflr(α)g(α)dαylr2+12x(1r1)(lr2)+ε(Q2r(r1)l2r(r1)+y2r(r1)l2r(r1)x(1r1)(2r(r1)l2r(r1))).

    Proof. The Cauchy's inequality gives us that

    mflr(α)g(α)dαsupαm|fr(α)|l2r1(10|fr(α)|2rdα)12(10g2(α)dα)12.

    We now use the result of [16] and get

    {supαmfr(α)yx1+1r+ε(Q1+y1x11r)12r1,if3r7,supαmfr(α)yx1+1r+ε(Q1+y1x11r)12r(r1),ifr8. (3.2)

    From that Lemma 2.5, Lemma 2.6 and (3.2), we get result of Lemma 3.1.

    By the definition of major arcs, we clearly have

    Mflr(α)g(α)dα=qQ1aq(a,q)=1M(q,a)flr(α)g(α)dα=qQ1aq(a,q)=1|λ|1qτflr(aq+λ)g(aq+λ)dλ. (3.3)

    By (2.1), Lemmas 2.2 and 2.4, we can conclude that

    flr(α)=Slr(q,a)qlTlr(N1r1,N1r2)+O(q1lrmin(yl1x(1+1r)(l1),1x(11r)(l1)||λ||l1)(1+|λ|y)).

    This combined with Lemma 2.7 gives that

    flr(α)g(α)=U(q,λ)+O(1+2),

    where

    U(q,λ)=Slr(q,a)qlTlr(N1r1,N1r2)k1j=0Aj(q)Ij(λ),

    and

    1=|flr(α)|(Qk+ε+yη+εQ),
    2=(q1lrmin(yl1x(1+1r)(l1),1x(11r)(l1)||λ||l1)(1+|λ|y))|k1j=0Aj(q)Ij(λ)|.

    Taking these into (3.3), we obtain

    Mflr(α)g(α)dα=qQ1aq(a,q)=1|λ|1qτU(q,λ)dλ+U1+U2,

    where the error terms Ui(i=1,2) satisfy

    UiqQ1aq(a,q)=1|λ|1qτidλ.

    The estimate of U1 will be separated into two cases.

    If 2r1<l<2r, it can be obtained by Hölder's inequality and Lemma 2.6 that

    qQ1aq(a,q)=1|λ|1qτ1dλ=(Qk+ε+yη+εQ)M|fr(α)|ldα(Qk+ε+yη+εQ)(10|fr(α)|2rdα)l2ry(1r2r)lx(1r1)(1r2r)l+εQk+ε+y(1r2r)l+ηx(1r1)(1r2r)l+εQ.

    If l2r, by Lemma 2.6, we have

    qQ1aq(a,q)=1|λ|1qτ1dλ=(Qk+ε+yη+εQ)M|fr(α)|ldα(Qk+ε+yη+εQ)supαI|fr(α)|l2r(10|fr(α)|2rdα)ylrx(lr)(1r1)+εQk+ε+ylr+ηx(lr)(1r1)+εQ.

    By (1.3) and (2.4), we have

    qQ1aq(a,q)=1|λ|1qτ2dλyl1x(1r1)(l1)qQq1lr1aq(a,q)=1k1j=0|Aj(q)||λ|1qτ|Ij(λ)|1+λy|dλylx(1r1)(l1)τ1yεqQqlrylx(1r1)(l1)+ετ1Qlr+1.
    qQ1aq(a,q)=1|λ|1qτU(q,λ)dλ=qQ1aq(a,q)=1Slr(q,a)qlk1j=0Aj(q)|λ|1qτIj(λ)Tlr(N1r1,N1r2)dλ.

    By means of (2.3) and (2.4), we have

    Ij(λ)Tlr(N1r1,N1r2)=1j!T(lN1,lN2)Tlr(N1r1,N1r2)+O(|Tr(N1r1,N1r2)|llogj(lN2)(1+y|λ|)).

    First, according to (1.3), (2.1) and Lemma 2.2, the contribution of the O-term to the integrals over the major arcs is

    qQ1aq(a,q)=1Slr(q,a)qlk1j=0Aj(q){1y0ylxl+lrlogj(lN2)(1+y|λ|)dλ+1qτ1yxl+lrλllogj(lN2)(1+y|λ|)dλ}qQ1aq(a,q)=1Slr(q,a)qlk1j=0Aj(q)xl+lr+εyl1yl1xl+lr+εQlr+1. (3.4)

    Hence, combining (3.4) and integrating over the major arcs, we obtain

    qQ1aq(a,q)=1|λ|1qτU(q,λ)dλ=qQ1aq(a,q)=1Slr(q,a)qlk1j=0Aj(q)1j!|λ|1qτT(lN1,lN2)Tlr(N1r1,N1r2)dλ+O(yl1xl+lr+εQlr+1). (3.5)

    In the integral of above identity, we extend the interval to [12,12]. By (2.1) and (2.2)

    121qτT(lN1,lN2)Tlr(N1r1,N1rr)dλ121qτxlrl(logx)λl1dλxlrlqlτl(logx). (3.6)

    Noting the condition (1.3), (3.1) and Lemma 2.2, the contribution of the above upper bound to the integrals over the major arcs is

    qQxlrlqllrτl(logx)xlrlτlQllr+1logxylxlrlε. (3.7)

    From (3.4) – (3.7), we have

    qQ1aq(a,q)=1|λ|1qτU(q,λ)dλ=qQ1aq(a,q)=1Slr(q,a)qlk1j=0Aj(q)1j!S(x,y)+O(yl1xl+lr+εQlr+1)+O(ylxlrlε),

    where

    S(x,y)=1212T(lN1,lN2)Tlr(N1r1,N1r2)dλ=1rlN1niN2i=1,2l1(n1ni)11rlN1nlN2n1+n2++nl=nlogjnlogjxN1niN2i=1,2l1(n1ni)11rylxl+lrlogjx.

    Therefore, we have established the following identity

    qQ1aq(a,q)=1|λ|1qτU(q,λ)dλ=q=11aq(a,q)=1Slr(q,a)qlk1j=0Aj(q)1j!S(x,y)+O(ylxl+lr(logjx)q>Qqlr)+O(yl1xl+lr+εQlr+1)+O(ylxl+lrε)=q=11aq(a,q)=1Slr(q,a)qlk1j=0Aj(q)1j!S(x,y)+O(ylxl+lrε). (3.8)

    By § 3.1.1, § 3.1.2 and (3.8), we get the following lemma.

    Lemma 3.2. For αM, let k2, r3, l>2r1 be integers.

    For 2r1<l<2r, we have

    Mflr(α)g(α)dα=q=11aq(a,q)=1Slr(q,a)qlk1j=0Aj(q)1j!S(x,y)+O(ylxl+lrε)++O(y(1r2r)lx(1r1)(1r2r)lQk+ε)+O(y(1r2r)l+ηx(1r1)(1r2r)l+εQ)+O(ylx(1r1)(l1)+ετ1Qlr+1).

    For l2r, we have

    Mflr(α)g(α)dα=q=11aq(a,q)=1Slr(q,a)qlk1j=0Aj(q)1j!S(x,y)+O(ylxl+lrε)++O(ylrx(lr)(1r1)+εQk+ε)+O(ylr+ηx(lr)(1r1)+εQ)+O(ylx(1r1)(l1)+ετ1Qlr+1),

    where Sr(q,a), Aj(q) and S(x,y) are defined in (1.1), (1.2) and (1.4), respectively.

    Finally, combining Lemma 3.1, Lemma 3.2 and noting that η=k1k+1 for 2k3 and η=k1k+2 for k4 by condition of Lemma 2.7, we can get the following that.

    Case 1. For 2r1<l<2r, 2k3, 3r7,

    Sk(x,y)=q=11aq(a,q)=1Slr(q,a)qlk1j=0Aj(q)1j!S(x,y)+O(ylxl+lrε)+O(y(1r2r)lx(1r1)(1r2r)l+εQk+ε)+O(y(1r2r)l+k1k+1x(1r1)(1r2r)l+εQ)+O(ylr2+12x(1r1)(lr2)+ε(Q2r1l2r1+y2r1l2r1x(1r1)(2r1l2r1)))+O(ylx(1r1)(l1)+ετ1Qlr+1).

    Case 2. For 2r1<l<2r, k4, 3r7,

    Sk(x,y)=q=11aq(a,q)=1Slr(q,a)qlk1j=0Aj(q)1j!S(x,y)+O(ylxl+lrε)+O(y(1r2r)lx(1r1)(1r2r)l+εQk+ε)+O(y(1r2r)l+k1k+2x(1r1)(1r2r)l+εQ)+O(ylr2+12x(1r1)(lr2)+ε(Q2r1l2r1+y2r1l2r1x(1r1)(2r1l2r1)))+O(ylx(1r1)(l1)+ετ1Qlr+1).

    Case 3. For l2r, 2k3, 3r7,

    Sk(x,y)=q=11aq(a,q)=1Slr(q,a)qlk1j=0Aj(q)1j!S(x,y)+O(ylxl+lrε)+O(ylrx(lr)(1r1)+εQk+ε)+O(ylr+k1k+1x(lr)(1r1)+εQ)+O(ylr2+12x(1r1)(lr2)+ε(Q2r1l2r1+y2r1l2r1x(1r1)(2r1l2r1)))+O(ylx(1r1)(l1)+ετ1Qlr+1).

    Case 4. For l2r, k4, 3r7,

    Sk(x,y)=q=11aq(a,q)=1Slr(q,a)qlk1j=0Aj(q)1j!S(x,y)+O(ylxl+lrε)++O(ylrx(lr)(1r1)+εQk+ε)+O(ylr+k1k+2x(lr)(1r1)+εQ)+O(ylr2+12x(1r1)(lr2)+ε(Q2r1l2r1+y2r1l2r1x(1r1)(2r1l2r1)))+O(ylx(1r1)(l1)+ετ1Qlr+1).

    Case 5. For 2r1<l<2r, 2k3, r8,

    Sk(x,y)=q=11aq(a,q)=1Slr(q,a)qlk1j=0Aj(q)1j!S(x,y)+O(ylxl+lrε)++O(y(1r2r)lx(1r1)(1r2r)l+εQk+ε)+O(y(1r2r)l+k1k+1x(1r1)(1r2r)l+εQ)+O(ylr2+12x(1r1)(lr2)+ε(Q2r(r1)l2r(r1)+y2r(r1)l2r(r1)x(1r1)(2r(r1)l2r(r1))))+O(ylx(1r1)(l1)+ετ1Qlr+1).

    Case 6. For 2r1<l<2r, k4, r8,

    Sk(x,y)=q=11aq(a,q)=1Slr(q,a)qlk1j=0Aj(q)1j!S(x,y)+O(ylxl+lrε)++O(y(1r2r)l+x(1r1)(1r2r)l+εQk+ε)+O(y(1r2r)l+k1k+2x(1r1)(1r2r)l+εQ)+O(ylr2+12x(1r1)(lr2)+ε(Q2r(r1)l2r(r1)+y2r(r1)l2r(r1)x(1r1)(2r(r1)l2r(r1))))+O(ylx(1r1)(l1)+ετ1Qlr+1).

    Case 7. For l2r, 2k3, r8,

    Sk(x,y)=q=11aq(a,q)=1Slr(q,a)qlk1j=0Aj(q)1j!S(x,y)+O(ylxl+lrε)++O(ylrx(lr)(1r1)+εQk+ε)+O(ylr+k1k+1x(lr)(1r1)+εQ)+O(ylr2+12x(1r1)(lr2)+ε(Q2r(r1)l2r(r1)+y2r(r1)l2r(r1)x(1r1)(2r(r1)l2r(r1))))+O(ylx(1r1)(l1)+ετ1Qlr+1).

    Case 8. For l2r, k4, r8,

    Sk(x,y)=q=11aq(a,q)=1Slr(q,a)qlk1j=0Aj(q)1j!S(x,y)+O(ylxl+lrε)++O(ylrx(lr)(1r1)+εQk+ε)+O(ylr+k1k+2x(lr)(1r1)+εQ)+O(ylr2+12x(1r1)(lr2)+ε(Q2r(r1)l2r(r1)+y2r(r1)l2r(r1)x(1r1)(2r(r1)l2r(r1))))+O(ylx(1r1)(l1)+ετ1Qlr+1).

    For Cases 1–4, we take y=xθ,θ=(11r)(r2+l2r1k2r1ε)r2+l2r1k2r112ε by condition of Theorem 1.1 and replace Q and τ in (3.1) by

    xεQ<τ, Qτyx11r, Q=y1kx1kr1k. (4.1)

    It is easy to see that

    ylr2+12x(1r1)(lr2)+εQ2r1l2r1>ylr2+12+2r1l2r1x(1r1)(lr2+2r1l2r1)+ε.

    In fact, we can check that the argument of Theorem 1.1 is valid if the parameters Q, τ and y satisfy the conditions

    max{y(1r2r)lx(1r1)(1r2r)l+εQk+ε,y(1r2r)l+k1k+1x(1r1)(1r2r)l+εQ}ylxl+lrε,max{ylrx(lr)(1r1)+εQk+ε,ylr+k1k+1x(lr)(1r1)+εQ}ylxl+lrε, (4.2)

    and

    ylr2+12x(1r1)(lr2)+εQ2r1l2r1ylxl+lrε,ylx(1r1)(l1)+ετ1Qlr+1ylxl+lrε.

    Therefore,

    Sk(x,y)=q=11aq(a,q)=1Slr(q,a)qlk1j=0Aj(q)1j!S(x,y)+O(ylxl+lrε).

    For Cases 4–8, we take y=xθ,θ=(11r)(r2+l2r(r1)k2r(r1)ε)r2+l2r(r1)k2r(r1)12ε by condition of Theorem 1.1. According to (4.1), we find

    ylr2+12x(1r1)(lr2)+εQ2r(r1)l2r(r1)>ylr2+12+2r(r1)l2r(r1)x(1r1)(lr2+2r(r1)l2r(r1))+ε.

    Actually, we can also deduce that Theorem 1.1 is available if the parameters Q, τ and y satisfying (4.2) and

    ylr2+12x(1r1)(lr2)+εQ2r(r1)l2r(r1)ylxl+lrε,ylx(1r1)(l1)+ετ1Qlr+1ylxl+lrε.

    Similarly,

    Sk(x,y)=q=11aq(a,q)=1Slr(q,a)qlk1j=0Aj(q)1j!S(x,y)+O(ylxl+lrε).

    This completes the proof of Theorem 1.1.

    The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.

    This work is supported by Natural Science Foundation of China (Grant Nos. 11761048), Natural Science Foundation of Jiangxi Province for Distinguished Young Scholars (Grant Nos. 20212ACB211007) and Natural Science Foundation of Jiangxi Province (Grant Nos. 20224BAB201001). The authors would like to express their thanks to the referee for many useful suggestions and comments on the manuscript.

    The authors declare there is no conflict of interests.



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