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Research article Special Issues

On mean square of the error term of a multivariable divisor function

  • Let τ(n) be the Dirichlet divisor function and k2 be a fixed integer. We give an asymptotic formula of the mean square of

    Δk(x)=n1,,nkxτ(n1nk)xkPk(logx).

    Citation: Zhen Guo. On mean square of the error term of a multivariable divisor function[J]. AIMS Mathematics, 2024, 9(10): 29197-29219. doi: 10.3934/math.20241415

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  • Let τ(n) be the Dirichlet divisor function and k2 be a fixed integer. We give an asymptotic formula of the mean square of

    Δk(x)=n1,,nkxτ(n1nk)xkPk(logx).



    Let τ(n) be the Dirichlet divisor function. It is known that for a real number x2,

    nxτ(n)=xlogx+(2γ1)x+Δ(x), (1.1)

    where γ is Euler's constant. It was first proved by Dirichlet that

    Δ(x)x.

    Let θ denotes the smallest number such that

    Δ(x)xθ+ε (1.2)

    holds for any ε>0. Many authors worked on making θ smaller, such as Voronoi [1], Corput [2], Kolesnik [3], Huxley [4], etc. Until now the best result, namely θ=131/416 is due to Huxley [4].

    It is conjectured that θ=1/4, which is supported by the classical mean square result: Suppose T is a large real number, then for any ε>0, one has

    T1Δ2(x)dx=16π2C2T3/2+O(T54+ε), (1.3)

    where

    C2=n=1τ2(n)n3/2.

    This result was given by Cramér [5] in 1922. In 1956, Tong [6] showed that the error term in (1.3) can be reduced to Tlog5T. In 1988, Preissmann [7] reduced the error term to Tlog4T. In 2009, Lau and Tsang [8] proved that

    T1Δ2(x)dx=16π2C2T3/2+O(Tlog3TloglogT).

    Let k2 be a fixed integer. Tóth and Zhai [9] considered the average of divisor function of k variables. They obtain the asymptotic formula

    n1,,nkxτ(n1nk)=xkPk(logx)+O(xk1+θ+ε) (1.4)

    holds for any ε>0, where θ is the exponent in (1.2) and Pk(t) is a polynomial in t of degree k. We denote Δk(x) by

    Δk(x):=n1,,nkxτ(n1nk)xkPk(logx). (1.5)

    We have the following theorem:

    Theorem 1.1. Suppose T2 is a large real number, then we have

    T1Δk2(x)dx=k24π2T2k12L2k2(logT)+O(T2k35+ε), (1.6)

    where L2k2(u) is a polynomial in u of degree 2k2, and the implied constant about "O" depends on k and ε.

    We present some lemmas.

    Lemma 2.1. Suppose x2 is large, then for any 1Nx, we have

    Δ(x)=x1/42πnNτ(n)n3/4cos(4πnxπ4)+O(x1/2+εN1/2).

    Proof. See [10,Chapter 3.2].

    Lemma 2.2. Suppose T2, TεyT, and let

    δ1(x,y)=x1/42πnyτ(n)n3/4cos(4πnxπ4),δ2(x,y)=Δ(x)δ1(x,y),

    then we have

    2TTδ22(x,y)dxT3/2y1/2log3T+Tlog4T.

    Proof. See, for example, the following references: Lau and Tsang [8], Tsang [11], Zhai [12].

    Lemma 2.3. Suppose G0,m0 are fixed real positive numbers, let G(x) be a monotonic function defined on [a,b] such that

    |G(x)|G0

    and m(x) be a differentiable real function such that

    |m(x)|m0

    on [a,b], F()=cos() or sin() or e(), then

    baG(x)F(m(x))dxG0m01.

    Proof. See [10,Lemma 2.1].

    Lemma 2.4. Let k2 be a fixed integer and let s1,,sk be complex numbers. Then for sj>1, where j=1,2,,k, we have

    n1,,nk=1τ(n1nk)ns11nskk=ζ2(s1)ζ2(sk)Fk(s1,,sk),

    where

    Fk(s1,,sk)=n1,,nk=1f(n1,,nk)ns11nskk.

    This series is absolutely convergent provided that sj>0 and (sj+sl)>1(1j,lk), and f(n1,,nk) is multiplicative and symmetric in all variables.

    Moreover, for r1,,rk{1,2},

    n1,,nk=1f(n1,,nk)τr1(n1)τrk(nk)ns11nskk (2.1)

    is absolutely convergent provided that sj>0 and (sj+sl)>1(1j,lk).

    Proof. See Tóth and Zhai [9,Proposition 2.1], and the convergence of (2.1) is a direct corollary.

    Lemma 2.5. Suppose x,y are large real numbers, k2 is a fixed integer, s,w are given real numbers such that 0<s<1/2<w<1, f is defined in Lemma 2.4. Let M1 and M2 denote the vectors (m1,,mk) and (mk+1,,m2k), D1 and D2 denote (k1j=1mj) and (2k1j=k+1mj), respectively. Let

    Tg,k(x,y;s,w)=m1,,m2kxn1,n2ymkm2k=n1n2f(M1)f(M2)g(M1,M2)D1D2(mkm2k)sτ(n1)τ(n2)(n1n2)w,Tg,k(s,w)=M1,M2Nkn1,n2Nmkm2k=n1n2f(M1)f(M2)g(M1,M2)D1D2(mkm2k)sτ(n1)τ(n2)(n1n2)w,

    where g(M1,M2) is any function that satisfies

    g(M1,M2)(2kj=1mj)ε,

    then we have:

    (i) Tg,k(s,w) is absolutely convergent.

    (ii) We have

    Tg,k(s,w)Tg,k(x,y;s,w)x2s+ε+y12wlog3y.

    Proof. (i) Since mk/m2k=n1/n2, we can find positive integers t1,t2,g1,g2 such that

    mkm2k=n1n2=t1t2,

    where (t1,t2)=1 and t1g1=mk, t2g1=m2k, t1g2=n1, t2g2=n2. Denote by M1 and M2 the vectors (m1,,mk1) and (mk+1,,m2k1), respectively, then we have

    Tg,k(s,w)M1,M2Nk1t1,t2,g1,g2N(t1,t2)=1|f(M1,t1g1)||f(M2,t2g1)||g(M1,t1g1,M2,t2g1)|τ(t1g2)τ(t2g2)D1D2(t1g1)s(t2g1)s(t1g2)w(t2g2)wM1,M2Nk1t1,t2,g1,g2N(t1,t2)=1|f(M1,t1g1)||f(M2,t2g1)||g(M1,t1g1,M2,t2g1)|τ(t1)τ(t2)τ2(g2)D1D2(t1g1)s(t2g1)s(t1t2)wg22wM1,M2Nk1t1,t2,g1N|f(M1,t1g1)||f(M2,t2g1)||g(M1,t1g1,M2,t2g1)|τ(t1)τ(t2)D1D2g12s(t1t2)s+wg2=1τ2(g2)g22wM1,M2Nk1t1,t2,g1N|f(M1,t1g1)||f(M2,t2g1)||g(M1,t1g1,M2,t2g1)|τ(t1)τ(t2)D1D2g12s(t1t2)s+w:=U1,

    where we use the conclusion: For a given real number c, we have

    n=1τ2(n)nc<(c>1), (2.2)

    moreover, for a large real number U, using partial summation and the conclusion

    nUτ2(n)Ulog3U,

    we have

    nUτ2(n)ncU21ucd(nuτ2(n))U1clog3U. (2.3)

    Since for any real δ>0,

    τ(n)/nδ1, (2.4)

    then

    U1=M1,M2Nk1t1,t2,g1N|f(M1,t1g1)||f(M2,t2g1)||g(M1,t1g1,M2,t2g1)|D1D2(t1g1)s(t2g1)sτ(t1)τ(t2)(t1t2)wM1,M2Nk1t1,t2,g1N|f(M1,t1g1)||f(M2,t2g1)||g(M1,t1g1,M2,t2g1)|D1D2(t1g1)s(t2g1)sM1,M2Nk1t1,t2,g1N|f(M1,t1g1)||f(M2,t2g1)|(D1D2)1ε(t1g1)sε(t2g1)sεM1,M2Nk1t1,t2,g1,g1N|f(M1,t1g1)||f(M2,t2g1)|(D1D2)1ε(t1g1)sε(t2g1)sε:=U2.

    Let t1g1=mk, t2g1=m2k, by Lemma 2.4, we have

    U2=M1,M2Nk1mk,m2kN|f(M1,mk)||f(M2,m2k)|τ(mk)τ(m2k)(D1D2)1εmksεm2ksε=(M1Nk1mkN|f(M1,mk)|τ(mk)D11εmksε)21.

    Thus, we conclude that (i) holds.

    (ii) Since m1,,mk1,mk+1,,m2k1 are symmetric, we have

    Tg,k(s,w)Tg,k(x,y;s,w)T1+T2+T3, (2.5)

    where

    T1=T1(x;s,w)=M1,M2Nkn1,n2Nmkm2k=n1n2m1>x|f(M1)||f(M2)||g(M1,M2)|D1D2mksm2ksτ(n1)τ(n2)n1wn2w,T2=T2(x;s,w)=M1,M2Nkn1,n2Nmkm2k=n1n2mk>xorm2k>x|f(M1)||f(M2)||g(M1,M2)|D1D2mksm2ksτ(n1)τ(n2)n1wn2w,T3=T3(y;s,w)=M1,M2Nkn1,n2Nmkm2k=n1n2n1>yorn2>y|f(M1)||f(M2)||g(M1,M2)|D1D2mksm2ksτ(n1)τ(n2)n1wn2w.

    Similar to (i), let (t1,t2)=1 and t1g1=mk, t2g1=m2k, t1g2=n1, t2g2=n2, and denote by M1 and M2 the vectors (m1,,mk1) and (mk+1,,m2k1) respectively, then

    T1=M1,M2Nk1t1,t2,g1,g2N(t1,t2)=1m1>x|f(M1,t1g1)||f(M2,t2g1)||g(M1,t1g1,M2,t2g1)|τ(t1g2)τ(t2g2)D1D2(t1g1)s(t2g1)s(t1g2)w(t2g2)wM1,M2Nk1t1,t2,g1,g2N(t1,t2)=1m1>x|f(M1,t1g1)||f(M2,t2g1)||g(M1,t1g1,M2,t2g1)|τ(t1)τ(t2)τ2(g2)D1D2(t1g1)s(t2g1)s(t1t2)wg22wM1,M2Nk1t1,t2,g1Nm1>x|f(M1,t1g1)||f(M2,t2g1)||g(M1,t1g1,M2,t2g1)|τ(t1)τ(t2)D1D2g12s(t1t2)s+wg2=1τ2(g2)g22wM1,M2Nk1t1,t2,g1Nm1>x|f(M1,t1g1)||f(M2,t2g1)||g(M1,t1g1,M2,t2g1)|τ(t1)τ(t2)D1D2g12s(t1t2)s+w:=T1, (2.6)

    where we use (2.2).

    Let

    D1=D1/m1,

    by (2.4), we have

    T1=M1,M2Nk1t1,t2,g1Nm1>x|f(M1,t1g1)||f(M2,t2g1)||g(M1,t1g1,M2,t2g1)|τ(t1)τ(t2)D1D2(t1g1)2s3ε(t2g1)3εt1ws+3εt2s+w3εM1,M2Nk1t1,t2,g1Nm1>x|f(M1,t1g1)||f(M1,t2g1)||g(M1,t1g1,M2,t2g1)|D1D2(t1g1)2s3ε(t2g1)3εM1,M2Nk1t1,t2,g1Nm1>x|f(M1,t1g1)||f(M2,t2g1)|m11εD11εD21ε(t1g1)2s4ε(t2g1)2εM1,M2Nk1t1,t2,g1,g1Nm1>x|f(M1,t1g1)||f(M2,t2g1)|m11εD11εD21ε(t1g1)2s4ε(t2g1)2ε:=T1. (2.7)

    Let t1g1=mk, t2g1=m2k, we have

    T1=M1,M2Nk1mk,m2kNm1>x|f(M1,mk)||f(M2,m2k)|τ(mk)τ(m2k)m112s+5εD11εD21εmk2s4εm2k2ε1m12s6εx2s+6εM1,M2Nk1mk,m2kN|f(M1,mk)||f(M2,m2k)|τ(mk)τ(m2k)m112s+5εD11εD21εmk2s4εm2k2εx2s+6εM1Nk1mkN|f(M1,mk)|τ(mk)m112s+5εD11εmk2s4εM1Nk1mkN|f(M1,mk)|τ(mk)D11εmk2εx2s+ε,

    the convergence of the two series in the last step can be obtained by Lemma 2.4, and we use the arbitrariness of ε.

    For T2, if mk>x, we replace the condition "m1>x" by "t1g1>x" in (2.6), thus

    T2M1,M2Nk1t1,t2,g1Nt1g1>x|f(M1,t1g1)||f(M2,t2g1)||g(M1,t1g1,M2,t2g1)|τ(t1)τ(t2)D1D2g12s(t1t2)s+w:=T2.

    Using (2.4) we have

    T2=M1,M2Nk1t1,t2,g1Nt1g1>x|f(M1,t1g1)||f(M2,t2g1)||g(M1,t1g1,M2,t2g1)|τ(t1)τ(t2)D1D2(t1g1)2s3ε(t2g1)3εt1ws+3εt2s+w3εM1,M2Nk1t1,t2,g1Nt1g1>x|f(M1,t1g1)||f(M2,t2g1)||g(M1,t1g1,M2,t2g1)|D1D2(t1g1)2s3ε(t2g1)3εM1,M2Nk1t1,t2,g1Nt1g1>x|f(M1,t1g1)||f(M2,t2g1)|(D1D2)1ε(t1g1)2s4ε(t2g1)2εM1,M2Nk1t1,t2,g1,g1Nt1g1>x|f(M1,t1g1)||f(M2,t2g1)|(D1D2)1ε(t1g1)2s4ε(t2g1)2ε:=T2. (2.8)

    Let t1g1=mk, t2g1=m2k, we have

    T2=M1,M2Nk1mk,m2kNmk>x|f(M1,mk)||f(M2,m2k)|τ(mk)τ(m2k)(D1D2)1εmk2s4εm2k2ε1m12s6εx2s+6εM1,M2Nk1mk,m2kN|f(M1,mk)||f(M2,m2k)|τ(mk)τ(m2k)(D1D2)1εmk2s4εm2k2εx2s+6εM1Nk1mkN|f(M1,mk)|τ(mk)D11εmk2s4εM1Nk1mkN|f(M1,mk)|τ(mk)D11εmk2εx2s+ε,

    the convergence of the two series in the last step can be obtained by Lemma {2.4}, and we use the arbitrariness of ε. If m2k>x, exchange t1 and t2, we can also obtain

    T2x2s+ε.

    For T3, if n1>y, similar to (i), we obtain (t1,t2)=1 and t1g1=mk, t2g1=m2k, t1g2=n1, t2g2=n2, then

    T3=M1,M2Nk1t1,t2,g1,g2N(t1,t2)=1t1g2>y|f(M1,t1g1)||f(M2,t2g1)||g(M1,t1g1,M2,t2g1)|τ(t1g2)τ(t2g2)D1D2(t1g1)s(t2g1)s(t1g2)w(t2g2)wM1,M2Nk1t1,t2,g1,g2N(t1,t2)=1t1g2>y|f(M1,t1g1)||f(M2,t2g1)||g(M1,t1g1,M2,t2g1)|τ(t1)τ(t2)τ2(g2)D1D2(t1g1)s(t2g1)s(t1t2)wg22wM1,M2Nk1t1,t2,g1N|f(M1,t1g1)||f(M2,t2g1)||g(M1,t1g1,M2,t2g1)|τ(t1)τ(t2)D1D2g12s(t1t2)s+wg2>yt1τ2(g2)g22wy12wlog3yM1,M2Nk1t1,t2,g1N|f(M1,t1g1)||f(M2,t2g1)||g(M1,t1g1,M2,t2g1)|τ(t1)τ(t2)D1D2g12st11+swt2s+w,

    where we use (2.3) by taking U=y/t1.

    We denote the latter series by Σ, using (2.4) we have

    Σ=M1,M2Nk1t1,t2,g1N|f(M1,t1g1)||f(M2,t2g1)||g(M1,t1g1,M2,t2g1)|τ(t1)τ(t2)D1D2(t1g1)s(t2g1)st11wt2wM1,M2Nk1t1,t2,g1N|f(M1,t1g1)||f(M2,t2g1)||g(M1,t1g1,M2,t2g1)|D1D2(t1g1)s(t2g1)sM1,M2Nk1t1,t2,g1N|f(M1,t1g1)||f(M2,t2g1)|(D1D2)1ε(t1g1)sε(t2g1)sεM1,M2Nk1t1,t2,g1,g1N|f(M1,t1g1)||f(M2,t2g1)|(D1D2)1ε(t1g1)sε(t2g1)sε.

    Let t1g1=mk, t2g1=m2k, we obtain

    ΣM1,M2Nk1mk,m2kN|f(M1,mk)||f(M1,m2k)|τ(mk)τ(m2k)(D1D2)1εmksεm2ksε=(M1Nk1mkN|f(M1,mk)|τ(mk)D11εmksε)21

    by Lemma 2.4, thus

    T3y12wlog3y.

    If n2>y, exchange t1 and t2, similarly we obtain

    T3y12wlog3y.

    Above all, we obtain

    T1,T2x2s+εandT3y12wlog3y,

    then (ii) holds from (2.5).

    We shall give a more explicit expression of Δk(x). According to Lemma 2.4,

    τ(n1nk)=m1d1=n1,,mkdk=nkf(m1,,mk)τ(d1)τ(dk)

    holds for any n1,,nkN, where f is multiplicative and symmetric in all variables.

    Therefore, we deduce by (1.1) that

    n1,,nkxτ(n1nk)=m1,,mkxf(m1,,mk)kj=1(djx/mjτ(dj))=m1,,mkxf(m1,,mk)kj=1(M(xmj)+Δ(xmj))=m1,,mkxf(m1,,mk)(kj=1M(xmj))+km1,,mkxf(m1,,mk)(k1j=1M(xmj))Δ(xmk)+(k2)m1,,mkxf(m1,,mk)(k2j=1M(xmj))Δ(xmk)Δ(xmk1)++(kk1)m1,,mkxf(m1,,mk)M(xm1)(kj=2Δ(xmj))+m1,,mkxf(m1,,mk)(kj=1Δ(xmj)):=m1,,mkxf(m1,,mk)(kj=1M(xmj))+E(x), (3.1)

    where

    M(u)=ulogu+(2γ1)u. (3.2)

    Here we have

    m1,,mkxf(m1,,mk)kj=1(M(xmj))=m1,,mk=1f(m1,,mk)kj=1(M(xmj))+O(xk1+ε)=xkPk(logx)+O(xk1+ε) (3.3)

    by the proof of Theorem 3.4 in Tóth and Zhai [9]. From (1.2) we have

    Δ(xmj)(xmj)θ+ε

    for any 1jk, then

    E(x)m1,,mkx|f(m1,,mk)|(k2j=1M(xmj))Δ(xmk)Δ(xmk1)xk2+2θ+εm1,,mkx|f(m1,,mk)|m1mk2(mk1mk)θ(mk1mk)12θ+ε(mk1mk)12θ+εxk2+2θ+ε(x2)12θ+εm1,,mk=1|f(m1,,mk)|m1mk2(mk1mk)12+εxk1+ε, (3.4)

    where the convergence of latter series can be obtained by Lemma 2.4. Then we conclude that

    Δk(x)=Δk(x)+O(xk1+ε) (3.5)

    follows by (1.4), (3.1), (3.3), and (3.4), where

    Δk(x)=km1,,mkxf(m1,,mk)(k1j=1M(xmj))Δ(xmk).

    Suppose T2, we shall first estimate 2TT(Δk(x))2dx. Since m1,,mk1 are symmetric, we can divide Δk(x) into three parts,

    Δk(x)=M1+O(M2+M3),

    where the implied constant about "O" depends on k and ε,

    M1=M1(x,y):=km1,,mkyf(m1,,mk)k1j=1M(xmj)Δ(xmk),M2=M2(x,y):=m1,,mkxm1>y|f(m1,,mk)|k1j=1M(xmj)|Δ(xmk)|,M3=M3(x,y):=m1,,mkxmk>y|f(m1,,mk)|k1j=1M(xmj)|Δ(xmk)|, (4.1)

    where y is a parameter that satisfies TεyT. So we obtain

    2TT(Δk(x))2dx=2TTM12dx+O(2TT(M1M2+M2M3+M1M3)dx)+O(2TT(M22+M32)dx). (4.2)

    First, we deal with 2TTM12dx. By Lemma 2.1 we obtain

    M1(x,y)=km1,,mkyf(m1,,mk)k1j=1M(xmj)(δ1(xmk,y)+δ2(xmk,y)):=M11(x,y)+M12(x,y),

    where

    M11(x,y)=km1,,mkyf(m1,,mk)k1j=1M(xmj)δ1(xmk,y),M12(x,y)=km1,,mkyf(m1,,mk)k1j=1M(xmj)δ2(xmk,y),

    and δ1(,y) and δ2(,y) are defined in Lemma 2.2, thus we have

    2TTM12(x,y)dx=2TTM112(x,y)dx+O(2TT(M11(x,y)M12(x,y)+M122(x,y))dx). (4.3)

    Let M1,M2 be defined in Lemma 2.5, using

    cosαcosβ=12(cos(αβ)+cos(α+β)),

    we have

    M112(x,y)=k2m1,,m2kyf(M1)f(M2)k1j=1M(xmj)2k1j=k+1M(xmj)×x1/22π2(mkm2k)1/4n1,n2yτ(n1)τ(n2)n13/4n23/4cos(4πn1xmkπ4)cos(4πn2xm2kπ4)=k2m1,,m2kyf(M1)f(M2)k1j=1M(xmj)2k1j=k+1M(xmj)x1/24π2(mkm2k)1/4×n1,n2yτ(n1)τ(n2)n13/4n23/4[cos(4π(n1mkn2m2k)x)+sin(4π(n1mk+n2m2k)x)]:=k2(S0(x,y)+S1(x,y)+S2(x,y)), (4.4)

    where

    S0(x,y)=x1/24π2m1,,m2kyf(M1)f(M2)(mkm2k)1/4k1j=1M(xmj)2k1j=k+1M(xmj)n1,n2yn1m2k=n2mkτ(n1)τ(n2)n13/4n23/4,S1(x,y)=x1/24π2m1,,m2kyf(M1)f(M2)(mkm2k)1/4k1j=1M(xmj)2k1j=k+1M(xmj)×n1,n2yn1m2kn2mkτ(n1)τ(n2)n13/4n23/4cos(4π(n1mkn2m2k)x),S2(x,y)=x1/24π2m1,,m2kyf(M1)f(M2)(mkm2k)1/4k1j=1M(xmj)2k1j=k+1M(xmj)×n1,n2yτ(n1)τ(n2)n13/4n23/4sin(4π(n1mk+n2m2k)x).

    So, it turns to evaluate

    0=2TTS0(x,y)dx,  1=2TTS1(x,y)dx,  2=2TTS2(x,y)dx.

    We need to give more explicit expressions for (k1j=1M(xmj)) and (2k1j=k+1M(xmj)). By the proof of Theorem 3.3 in Tóth and Zhai [9] in the case fj(n)=τ(n),aj=1,δj=1(1jk1) we obtain

    k1j=1M(xmj)=xk1m1mk1k1l1=0Cl1(logm1,,logmk1)(logx)l1, (4.5)

    where

    Cl1(logm1,,logmk1)=j1,,jk1=0,1c(j1,,jk1)(logm1)j1(logmk1)jk1,

    and c(j1,,jk1) are constants (j1,,jk1=0,1). Similarly, when k+1j2k1, we have

    2k1j=k+1M(xmj)=xk1mk+1m2k12k1l2=kCl2(logmk+1,,logm2k1)(logx)l2k, (4.6)

    where

    Cl2(logmk+1,,logm2k1)=jk+1,,j2k1=0,1c(jk+1,,j2k1)(logmk+1)jk+1(logm2k1)j2k1,

    and c(jk+1,,j2k1) are constants (jk+1,,j2k1=0,1).

    We denote Cl1(logm1,,logmk1)Cl2(logmk+1,,logm2k1) by Cl1,l2(M1,M2), using (4.5) and (4.6) we have

    S0(x,y)=x2k324π2k1l1,l2=0(logx)l1+l2m1,,m2kyn1,n2ymkm2k=n1n2f(M1)f(M2)Cl1,l2(M1,M2)D1D2(mkm2k)14τ(n1)τ(n2)(n1n2)34, (4.7)

    where D1,D2 are defined in Lemma 2.5. Using (2.4) we obtain

    Cl1,l2(M1,M2)(k1j=1mj2k1j=k+1mj)ε(2kj=1mj)ε.

    Choosing

    g(M1,M2)=gl1,l2(M1,M2)=Cl1,l2(M1,M2),

    s=1/4, w=3/4 in Lemma 2.5, we obtain that S0(x,y) can be written as

    S0(x,y)=x2k324π2k1l1,l2=0(logx)l1+l2×Tg,k(y,y;14,34)=x2k324π2k1l1,l2=0(logx)l1+l2(Tg,k(14,34)+O(y12+ε)). (4.8)

    Since g(M1,M2) is related to l1,l2, we denote Tg,k(14,34) in (4.8) by Dk,l1,l2, we conclude that

    S0(x,y)=x2k324π2Q2k2(logx)+O(x2k32+εy12+ε), (4.9)

    where

    Q2k2(t)=k1l1,l2=0Dk,l1,l2tl1+l2.

    Then it follows from (4.9) that

    2TTS0(x,y)dx=14π2k1l1,l2=0Dk,l1,l22TTx2k32(logx)l1+l2dx+O(T2k12+εy12). (4.10)

    Let M1,M2,D1,D2 be defined in Lemma 2.5, then by (4.5) and (4.6) we have

    2=2TTx2k324π2k1l1,l2=0(logx)l1+l2m1,,m2kyCl1,l2(M1,M2)D1D2×n1,n2yf(M1)f(M2)mk1/4m2k1/4τ(n1)τ(n2)n13/4n23/4sin(4π(n1mk+n2m2k)x)dx.

    Let

    G(x)=x2k32(logx)l1+l2,   F()=sin(),   m(x)=4π(n1mk+n2m2k)x,   a=T,  b=2T

    in Lemma 2.3, change the order of integration and summation, then we have

    2=14π2k1l1,l2=0m1,,m2kyn1,n2yCl1,l2(M1,M2)D1D2f(M1)f(M2)mk1/4m2k1/4τ(n1)τ(n2)n13/4n23/4×2TTx2k32(logx)l1+l2sin(4π(n1mk+n2m2k)x)dxm1,,m2kyn1,n2y|Cl1,l2(M1,M2)|D1D2|f(M1)||f(M2)|mk1/4m2k1/4τ(n1)τ(n2)n13/4n23/4×T2k32+εT12n1mk+n2m2k,

    then we use

    a2+b22ab,   Cl1,l2(M1,M2)(2kj=1mj)ε

    to obtain

    2T2k1+εm1,,m2kyn1,n2y(2kj=1mj)εD1D2|f(M1)||f(M2)|mk1/4m2k1/4τ(n1)τ(n2)n13/4n23/4(mkm2kn1n2)14T2k1+(2k+1)εm1,,m2kyn1,n2y|f(M1)||f(M2)|D1D2τ(n1)τ(n2)n1n2T2εmkεm2kεT2k1+(2k+3)εm1,,m2k=1|f(M1)||f(M2)|D1D2mkεm2kεn1,n2yτ(n1)τ(n2)n1n2T2k1+(2k+4)ε(m1,,m2k=1|f(M1)|D1mkε)2,

    where by partial summation we obtain

    n1,n2yτ(n1)τ(n2)n1n2log4ylog4TTε.

    Since ε>0 is arbitrary, using Lemma 2.4 we conclude that

    2T2k1+ε. (4.11)

    Then we turn to estimate 1, similar to 2, we have

    1=2TTx2k324π2k1l1,l2=0(logx)l1+l2m1,,m2kyCl1,l2(M1,M2)D1D2×n1,n2yn1m2kn2mkf(M1)f(M2)mk1/4m2k1/4τ(n1)τ(n2)n13/4n23/4cos(4π(n1mkn2m2k)x)dx.

    Let

    G(x)=x2k32(logx)l1+l2,   F()=cos(),   m(x)=4π(n1mkn2m2k)x,   a=T,  b=2T

    in Lemma 2.3, change the order of integration and summation, then we have

    1=14π2k1l1,l2=0m1,,m2kyCl1,l2(M1,M2)D1D2f(M1)f(M2)mk1/4m2k1/4n1,n2yn1m2kn2mkτ(n1)τ(n2)n13/4n23/4×2TTx2k32(logx)l1+l2cos(4π(n1mkn2m2k)x)dxk1l1,l2=0m1,,m2ky|Cl1,l2(M1,M2)|D1D2|f(M1)||f(M2)|mk1/4m2k1/4n1,n2y2n1m2kn2mkτ(n1)τ(n2)n13/4n23/4×T2k32+εT12|n1mkn2m2k|.

    Since

    Cl1,l2(M1,M2)(2kj=1mj)ε,

    we have

    1T2k1+εm1,,m2ky(2kj=1mj)εD1D2|f(M1)||f(M2)|mk1/4m2k1/4n1,n2yn1m2kn2mkτ(n1)τ(n2)n13/4n23/41|n1mkn2m2k|T2k1+(2k+1)εm1,,m2ky|f(M1)||f(M2)|D1D2mk1/4m2k1/4n1,n2yn1m2kn2mkτ(n1)τ(n2)n13/4n23/41|n1mkn2m2k|:=T2k1+(2k+1)εm1,,m2ky|f(M1)||f(M2)|D1D2mk1/4m2k1/4(R1+R2), (4.12)

    where

    R1=n1,n2y,n1m2kn2mk|n1mkn2m2k|(n1n2)1/410(mkm2k)1/4τ(n1)τ(n2)n13/4n23/41|n1mkn2m2k|,R2=n1,n2y,n1m2kn2mk|n1mkn2m2k|>(n1n2)1/410(mkm2k)1/4τ(n1)τ(n2)n13/4n23/41|n1mkn2m2k|.

    Then we have

    R2n1,n2yτ(n1)τ(n2)n13/4n23/4(mkm2k)1/4(n1n2)1/4(mkm2k)14log4T, (4.13)

    where we use partial summation to obtain

    n1,n2yτ(n1)τ(n2)n1n2log4ylog4T.

    And for R1, by Lagrange's mean value theorem we have

    β1β2(β1β2)12|β1β2|

    for any

    β1β2R,

    thus let

    β1=n1/mk,   β2=n2/m2k

    in R1, we obtain

    R1n1,n2yn1m2kn2mkτ(n1)τ(n2)n13/4n23/41|n1mkn2m2k|(mkm2kn1n2)1/4=(mkm2k)34n1,n2yn1m2kn2mkτ(n1)τ(n2)n1/21n1/22|n1m2kn2mk|.

    For some real numbers N1, N2 satisfying 1N1,N2y, one has

    R1(mkm2k)34log2yN1<n12N1N2<n22N2n1m2kn2mkτ(n1)τ(n2)(n1n2)1/2|n1m2kn2mk|(mkm2k)34yε(N1N2)1/2N1<n12N1N2<n22N2n1m2kn2mk1|n1m2kn2mk|, (4.14)

    we denote the latter sum by T(mk,m2k). Let

    |n1m2kn2mk|=r,

    we have

    rn1m2k(mod mk),

    so we can find a constant c0 such that

    1c0<mk,   r=mkt+c0,

    where t is an integer such that 0<t<2y2, thus

    T(mk,m2k)=N1<n12N1N2<n22N2n1m2kn2mk1|n1m2kn2mk|N1<n12N1(1+1t2y21mkt+c0)N1logy,

    similarly, we have

    T(mk,m2k)N2logy,

    thus

    T(mk,m2k)(N1N2)12logy.

    By (4.14) we have

    R1(mkm2k)34yε(N1N2)1/2(N1N2)12logy(mkm2k)34Tε. (4.15)

    Finally by (4.12), (4.13) and (4.15) we obtain

    R1+R2Tε(mkm2k)3/4,

    thus

    1T2k1+(2k+1)εm1,,m2ky|f(M1)||f(M2)|D1D2mk1/4m2k1/4Tεmk3/4m2k3/4T2k1+(2k+2)εm1,,m2ky|f(M1)||f(M2)|mk1/2m2k1/2D1D2T2k1+(2k+2)εym1,,m2ky|f(M1)||f(M2)|D1D2T2εmkεm2kεT2k1+(2k+4)εy(m1,,mk=1|f(M1)|D1mkε)2T2k1+εy, (4.16)

    since ε>0 is arbitrary, TεyT, and the convergence of the latter series can be obtained by Lemma 2.4. Above all, by (4.4), (4.10), (4.11), and (4.16) we obtain

    2TTM112(x,y)dx=k24π2k1l1,l2=0Dk,l1,l22TTx2k32(logx)l1+l2dx+O(T2k12+εy12)+O(T2k1+εy). (4.17)

    We are going to estimate 2TTM12(x,y)dx,

    2TTM122(x,y)dx=k22TT(m1,,mkyf(M1)k1j=1M(xmj)δ2(xmk,y))2dx2TTm1,,m2ky|f(M1)||f(M2)|(k1j=1xlogxmj2k1j=k+1xlogxmj)|δ2(xmk,y)||δ2(xm2k,y)|dxm1,,m2ky|f(M1)||f(M2)|D1D22TTx2k2+ε|δ2(xmk,y)||δ2(xm2k,y)|dxT2k2+εm1,,m2ky|f(M1)||f(M2)|D1D2(2TTδ22(xmk,y)dx)12(2TTδ22(xm2k,y)dx)12. (4.18)

    By Lemma 2.2 we have

    (2TTδ22(xmk,y)dx)12=(mk2TmkTmkδ22(u,y)du)12(mk(T32mk32y12log3T+Tmklog4T))12T34+εmk14y14+T12+ε,

    similarly, we have

    (2TTδ22(xm2k,y)dx)12T34+εm2k14y14+T12+ε.

    Thus,

    2TTM122(x,y)dxT2k2+εm1,,m2ky|f(M1)||f(M2)|D1D2(T34+εmk14y14+T12+ε)(T34+εm2k14y14+T12+ε)T2k12+3εy12m1,,m2k=1|f(M1)||f(M2)|D1D2mk14m2k14T2k12+3εy12, (4.19)

    since yT, and the convergence of the latter series is given by Lemma 2.4.

    Then by (4.17), (4.19), and Cauchy-Schwarz's inequality, we are able to obtain

    2TTM11M12dx(2TTM112dx)12(2TTM122dx)12T2k12+εy14. (4.20)

    So from (4.3) and (4.17)–(4.20), we obtain

    2TTM12dx=k24π2k1l1,l2=0Dk,l1,l22TTx2k32(logx)l1+l2dx+O(T2k12+εy14)+O(T2k1+εy). (4.21)

    Let M1,M2,D1,D2 be defined in Lemma 2.5, then for 2TTM32dx we deduce that

    2TTM32(x,y)dx=2TT(m1,,mkxmk>y|f(m1,,mk)|k1j=1M(xmj)|Δ(xmk)|)2dx

    change order of integration and summation we obtain

    2TTM32(x,y)dx2TTm1,,m2k2Tmk,m2k>y|f(M1)f(M2)|k1j=1M(xmj)2k1j=k+1M(xmj)|Δ(xmk)||Δ(xm2k)|dx=m1,,m2k2Tmk,m2k>y|f(M1)f(M2)|2TTk1j=1M(xmj)2k1j=k+1M(xmj)|Δ(xmk)||Δ(xm2k)|dxm1,,m2k2Tmk,m2k>y|f(M1)||f(M2)|D1D22TTx2k2+ε|Δ(xmk)||Δ(xm2k)|dxT2k2+εm1,,m2k2Tmk,m2k>y|f(M1)||f(M2)|D1D22TT|Δ(xmk)||Δ(xm2k)|dx.

    Using Cauchy-Schwarz's inequality and (1.3), we deduce that

    2TT|Δ(xmk)||Δ(xm2k)|dx(2TTΔ2(xmk)dx)12(2TTΔ2(xm2k)dx)12(mk2TmkTmkΔ2(u)du)12(m2k2Tm2kTm2kΔ2(u)du)12T32mk14m2k14,

    thus, by Lemma 2.4, we have

    2TTM32(x,y)dxT2k12+εm1,,m2k2Tmk,m2k>y|f(M1)||f(M2)|D1D2mk14m2k14T2k12+εm1,,m2k2Tmk,m2k>y|f(M1)||f(M2)|D1D2mkεm2kεmk14+εm2k14+εT2k12+εy12+2εm1,,m2k2Tmk,m2k>y|f(M1)||f(M2)|D1D2mkεm2kεT2k12+εy12m1,,m2k=1|f(M1)||f(M2)|D1D2mkεm2kεT2k12+εy12. (4.22)

    For 2TTM22dx, let D1=D1/m1, D2=D2/mk+1, similar to 2TTM32dx, we obtain by Lemma 2.4 that

    2TTM22(x,y)dxT2k12+εm1,,m2k2Tm1,mk+1>y|f(M1)||f(M2)|D1D2mk14m2k14T2k12+εm1,,m2k2Tm1,mk+1>y|f(M1)||f(M2)|m114+εmk+114+εD1D2m134+εmk14mk+134+εm2k14T2k12+εy12+2εm1,,m2k2Tm1,mk+1>y|f(M1)||f(M2)|D1D2m134+εmk14mk+134+εm2k14T2k12+εy12m1,,m2k=1|f(M1)||f(M2)|D1D2m134+εmk14mk+134+εm2k14T2k12+εy12. (4.23)

    By (4.21)–(4.23) and Cauchy-Schwarz's inequality, we are able to estimate the following terms in (4.2)

    2TTM1M2dx(2TTM12dx)12(2TTM22dx)12T2k12+εy14,2TTM1M3dx(2TTM12dx)12(2TTM32dx)12T2k12+εy14,2TTM2M3dx(2TTM22dx)12(2TTM32dx)12T2k12+εy12. (4.24)

    Above all, taking y=T25, then

    2TT(Δk(x))2dx=k24π2k1l1,l2=0Dk,l1,l22TTx2k32(logx)l1+l2dx+O(T2k35+ε) (4.25)

    follows by (4.2) and (4.21)–(4.24).

    Using (3.5) and the Cauchy-Schwarz's inequality we obtain

    2TTΔk2(x)dx=2TT(Δk(x))2dx+O(2TTΔk(x)xk1+εdx)+O(T2k1+ε)=k24π2k1l1,l2=0Dk,l1,l22TTx2k32(logx)l1+l2dx+O(T2k35+ε)+O((2TT(Δk(x))2dx)12(2TTx2k2+εdx)12)=k24π2k1l1,l2=0Dk,l1,l22TTx2k32(logx)l1+l2dx+O(T2k35+ε).

    Then replacing T by T/2, T/22, and so on, and adding up all the results, we obtain

    T1Δk2(x)dx=k24π2k1l1,l2=0Dk,l1,l2T1x2k32(logx)l1+l2dx+O(T2k35+ε)=k24π2T2k12L2k2(logT)+O(T2k35+ε),

    where we use integration by part several times to obtain L2k2(u) is a polynomial in u of degree 2k2 denoted by

    L2k2(u)=k1l1,l2=0Dk,l1,l2l1+l2r=0(1)r(l1+l2)!(2k12)r+1(l1+l2r)!ul1+l2.

    To sum up, this finishes the proof of the Theorem.

    In this paper, we give an asymptotic formula of the mean square of Δk(x), which can be viewed as an analogue of (1.3). We use the convergence of the multivariable Dirichlet series, and it can be used to show the properties of other multivariable arithmetic functions. In 2023, Tóth[13], Heyman and Tóth[14] gave some useful applications of the Dirichlet series.

    The author would like to appreciate the referee for his/her patience in refereeing this paper. This work is supported by Natural Science Foundation of Beijing Municipal (Grant No.1242003), and the National Natural Science Foundation of China (Grant Nos.12471009 and 12301006).

    No potential conflicts of interest were reported by the author.



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    沈阳化工大学材料科学与工程学院 沈阳 110142

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