Research article Special Issues

On two-term exponential sums and their mean values

  • The mean value problems of exponential sums play a very important role in the research of analytic number theory, and many famous number theory problems are closely related to them. The main purpose of this paper is using some elementary methods and the number of the solutions of the congruence equations to study the calculating problem of some fourth power means of two-term exponential sums, and give exact calculating formulae and asymptotic formula for them.

    Citation: Jianghua Li, Zepeng Zhang, Tianyu Pan. On two-term exponential sums and their mean values[J]. Electronic Research Archive, 2023, 31(9): 5559-5572. doi: 10.3934/era.2023282

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  • The mean value problems of exponential sums play a very important role in the research of analytic number theory, and many famous number theory problems are closely related to them. The main purpose of this paper is using some elementary methods and the number of the solutions of the congruence equations to study the calculating problem of some fourth power means of two-term exponential sums, and give exact calculating formulae and asymptotic formula for them.



    As usual, let p be an odd prime. For any integers h>r1 and integers m and n, the two-term exponential sum S(m,n,h,r;p) is defined as

    S(m,n,h,r;p)=p1a=0e(mah+narp),

    where e(y)=e2πiy and i is the imaginary unit. That is, i2=1.

    These sums play very important role in the study of analytic number theory, so many number theorists have studied the various properties of S(m,n,h,r;p) and obtained some meaningful research results. Here we give a few examples. W. P. Zhang and D. Han [1] used analytic methods to study the sixth power mean of S(1,m,3,1;p), and proved the following result:

    p1m=1|p1a=0e(a3+map)|6=5p48p3p2, (1.1)

    where p denotes an odd prime with 3(p1).

    Recently, W. P. Zhang and Y. Y. Meng [2] also studied the sixth power mean of S(m,n,3,1;p), and obtained some new identities. In fact, they proved that for any odd prime p and integer n with (n,p)=1, one has

    p1m=1|p1a=0e(ma3+nap)|6={5p3(p1)if p5mod6;p2(5p223pd2)if p1mod6. (1.2)

    here, 4p=d2+27b2, and d is uniquely determined by d1mod3.

    On the other hand, L. Chen and X. Wang [3] proved

    p1m=1|p1a=0e(ma4+ap)|4={2p2(p2)if p7mod12,2p3if p11mod12,2p(p210p2α2)if p1mod24,2p(p24p2α2)if p5mod24,2p(p26p2α2)if p13mod24,2p(p28p2α2)if p17mod24, (1.3)

    where the character sums α=α(p)=p12a=1(a3+ap) is an integer satisfying the identity (see Theorem 4–11 in [4]):

    p=α2+β2=(p12a=1(a3+ap))2+(p12a=1(a3+rap))2.

    (p) denotes the Legendre symbol, and r is a quadratic non-residue modulo p.

    In addition, some related papers can also be found in [5,6,7,8,9,10,11].

    From the formulae (1.1)–(1.3), it is not difficult to see that the content of all these papers only involves r=1 in S(m,n,h,r;p). For the case r>1 in S(m,n,h,r;p), we have not found a corresponding conclusion, at least not so far. Therefore, when h>r=2, the research is difficult, and it is difficult to obtain some ideal results.

    In this paper, we use elementary methods and results on the number of solutions to study the calculating problem of the 2k-th power mean

    S2k(p)=p1m=0|p1a=0e(ma4+a2p)|2k,

    and give an exact calculating formula for S4(p) with p3mod4. That is, we will prove the following two main results:

    Theorem 1. Let p be a prime with p3mod4. Then, we have the identity

    p1m=0|p1a=0e(ma4+a2p)|4=p2(7p10).

    Theorem 2. Let p be a prime with p1mod4. Then, we have the identity

      p1a=0p1b=0p1c=0a4+b4c4+1modp1=p2+13p+4(1)p14p2α(p)4(1)p14α(p)+4α2(p),

    where α=α(p) is defined in (1.3).

    Some notes: In Theorem 1, we only discussed a prime p in the case p3mod4. If p1mod4, then the situation is much more complicated. We cannot calculate the exact value of S4(p), and we cannot even get a valid asymptotic formula for S4(p). The reason is that we do not know the exact value of

    p1a=0p1b=0p1c=0a4+b4c4+1modp(a2+b2c21p) (1.4)

    and do not know a valid asymptotic formula for it.

    However, if p1mod4, we give some ideas and methods of studying S4(p) (see Lemma 3 and Lemma 4 below). We even have the following:

    Conjecture. If prime p1mod4, then there is an asymptotic formula

    p1m=0|p1a=0e(ma4+a2p)|4=7p3+O(p52).

    To prove this conjecture, we can convert (1.4) to the estimate for character sums

    p1a=0p1b=0p1c=0a2+b2c2+1modp(ab(a+bc1)p)

    or character sums

    D(p)=p1a=0p1c=0(ac(ac1)(a2c21)p).

    If one can give a non-trivial upper bound estimate for D(p), such as |D(p)|p, then we can prove that the conjecture is correct.

    For any odd prime p with p3mod4 and integer k3, whether there exists an exact calculating formula for

    p1m=0|p1a=0e(ma4+a2p)|2k

    is an open problem. Interested readers can continue this research.

    To complete the proofs of our main results, we need some simple lemmas. Of course, the proofs of all these lemmas need some knowledge of elementary number theory and analytic number theory, and all these can be found in [12,13], so we do not have to repeat them here. First, we have the following:

    Lemma 1. For any odd prime p, we have the identities

    p1a=0p1b=0p1c=0a4+b4c4+1modpa2+b2c2+1modp1=4(2p3)  and   p1a=0p1c=0a4+1c4modpa2+1c2modp1=2.

    Proof. It is clear that

    p1a=0p1b=0p1c=0a4+b4c4+1modpa2+b2c2+1modp1=p1a=0p1b=0p1c=0(a2+b2)2a4b4(c2+1)2c41modpa2+b2c2+1modp1=p1a=0p1b=0p1c=0a2b2c2modpa2+b2c2+1modp1=p1a=0p1b=0p1c=0(a21)(b21)0modpa2+b2c2+1modp1=4(p3)+2+4(p3)+2+8=4(2p3). (2.1)

    Similarly, we also have

    p1a=0p1c=0a4+1c4modpa2+1c2modp1=p1a=0p1c=0(a2+1)2a41c4c4modpa2+1c2modp1=p1a=0p1c=0a20modpa2+1c2modp1=2. (2.2)

    Now Lemma 1 follows from (2.1) and (2.2).

    Lemma 2. Let p be a prime with p3mod4. Then, we have the identities

    p1a=0p1c=0a4+1c4modp1=p1

    and

    p1a=0p1b=0p1c=0a4+b4c4+1modp1=p2+p.

    Proof. First, we prove the second formula in Lemma 2. Let ¯b denote the inverse of bmodp, i.e., b¯b1(modp). From the properties of a complete residue system modulo p, we have

    p1a=0p1b=0p1c=0a2+b2c2+1modp1=p1a=0p1b=0p1c=0(a+c)2+(b+1)2c2+1modp1=p1a=0p1b=0p1c=0a2+2ac+b2+2b0modp1=p1a=0p1b=1p1c=0a(a+2c)+1+2¯b0modp1+p1a=0p1c=0a(a+2c)0modp1=p1a=0p1b=0p1c=0ac+b0modp1p1a=0p1c=0ac+10modp1+(2p1)=p2(p1)+(2p1)=p2+p. (2.3)

    Since p3mod4, from the properties of the Legendre symbol modulo p, we have (1p)=1 and

    p1a=0p1b=0p1c=0a2+b2c2+1modp(ap)=p1a=0p1b=0p1c=0(a)2+b2c2+1modp(ap)=p1a=0p1b=0p1c=0a2+b2c2+1modp(ap)

    or

    p1a=0p1b=0p1c=0a2+b2c2+1modp(ap)=0. (2.4)

    Similarly, we also have

    p1a=0p1b=0p1c=0a2+b2c2+1modp(abp)=p1a=0p1b=0p1c=0a2+b2c2+1modp(acp)=p1a=0p1b=0p1c=0a2+b2c2+1modp(abcp)=0. (2.5)

    It is clear that we have the identity

    p1a=0p1b=0p1c=0a4+b4c4+1modp1=p1a=0p1b=0p1c=0a2+b2c2+1modp(1+(ap))(1+(bp))(1+(cp))=p1a=0p1b=0p1c=0a2+b2c2+1modp1+2p1a=0p1b=0p1c=0a2+b2c2+1modp(ap)+p1a=0p1b=0p1c=0a2+b2c2+1modp(cp)+2p1a=0p1b=0p1c=0a2+b2c2+1modp(acp)+p1a=0p1b=0p1c=0a2+b2c2+1modp(abp)+p1a=0p1b=0p1c=0a2+b2c2+1modp(abcp). (2.6)

    Combining (2.3)–(2.6), we have the identity

    p1a=0p1b=0p1c=0a4+b4c4+1modp1=p2+p.

    Similarly, we can also deduce the first formula in Lemma 2, which is

    p1a=0p1c=0a4+1c4modp1=p1a=0p1c=0a2+1c2modp(1+(ap))(1+(cp))=p1a=0p1c=0a2+1c2modp1+2p1a=0p1c=0a2+1c2modp(ap)+p1a=0p1c=0a2+1c2modp(acp).

    Using the method (2.3)–(2.6) and removing element b, we immediately get

    p1a=0p1c=0a4+1c4modp1=p1.

    This proves Lemma 2.

    Lemma 3. Let p be a prime with p1mod4. Then, we have the identity

    p1a=0p1b=0p1c=0a4+b4c4+1modp1=p2+13p+4(1)p14p2α(p)4(1)p14α(p)+4α2(p).

    Proof. The proof of the lemma is mainly divided into three parts:

    (ⅰ) Summing Legendre symbols containing one variable, we have

    p1a=0p1b=0p1c=0a2+b2c2+1modp(bp)=p1a=0p1b=0p1c=0a2+b2c2+1modp(ap)=p1a=0p1b=0p1c=0a2+b2+2bc1modp(ap)=p1a=0p1b=0p1c=0a2+b(b+2c)1modp(ap)=p1a=0p1b=0p1c=0a2+bc1modp(ap)=2p+p1a=0p1b=1p1c=0a2+c1modp(ap)=2p+(p1)p1a=1(ap)=2p. (2.7)

    Note the identities

    p1b=0(b2+np)={p1if pn,1if pn.

    We have

    p1a=0p1b=0p1c=0a2+b2c2+1modp(cp)=p1a=0p1b=0p1c=0a+b2c2+1modp(cp)(1+(ap))=p1b=0p1c=0(cp)+p1b=0p1c=0(cp)(c2+1b2p)=p1c=0(cp)p1b=0(b2c21p)=(p1)p1c=0p(c2+1)(cp)p1c=0p(c2+1)(cp)=pp1c=0p(c2+1)(cp)p1c=0(cp)=2(1)p14p. (2.8)

    (ⅱ) Summing Legendre symbols containing two variables, we can get

    p1a=0p1b=0p1c=0a2+b2c2+1modp(abp)=p1a=0p1b=1p1c=0(ab)2+b2(cb)2+1modp(ab2p)=p1a=0p1b=1p1c=0a2+1c2+¯b2modp(ap)=p1a=0p1b=0p1c=0b2+c2a2+1modp(ap)p1a=0p1c=0c2a2+1modp(ap)=2(1)p14pp1a=0(ap)(1+(1+a2p))=2(1)p14pp1a=1(a+¯ap)=2(1)p14p2α(p). (2.9)

    and

    p1a=0p1b=0p1c=0a2+b2c2+1modp(bcp)=p1a=0p1b=0p1c=0a2+b2c2+1modp(acp)=p1a=0p1b=0p1c=1(ac)2+(bc)2c2+1modp(ac2p)=p1a=0p1b=0p1c=1a2+b21+¯c2modp(ap)=p1a=0p1b=0p1c=0a2+b21+c2modp(ap)p1a=0p1b=0a2+b21modp(ap)=2pp1a=0(ap)(1+(1a2p))=2p2(1)p14α(p). (2.10)

    (ⅲ) Summing Legendre symbols containing three variables, we can obtain

    p1a=0p1b=0p1c=0a2+b2c2+1modp(abcp)=p1a=1p1b=1p1c=1b2a2+b2c2+1modp(ab2cp)=p1a=1p1b=1p1c=1b2(a2+1)c2+1modp(acp)=p1a=1p1b=1p1c=1a2+10modp(acp)+p1a=1p1b=1p1c=1(b(a2+1))2(a2+1)(c2+1)modp(a2+1,p)=1(acp)=(p1)(p1a=1a2+10modp(ap))2+p1a=1p1b=1p1c=1b2(a2+1)(c2+1)modp(acp)=4(p1)+p1a=1p1b=0p1c=1b2(a2+1)(c2+1)modp(acp)p1a=1p1c=1(a2+1)(c2+1)0modp(acp)=4p+p1a=1p1c=1(acp)(1+((a2+1)(c2+1)p))2(1)p14p1c=1(cp)=4p+(p1a=1(a+¯ap))2=4p+4α2(p). (2.11)

    Combining (2.3), (2.6)–(2.11) we have the identity

    p1a=0p1b=0p1c=0a4+b4c4+1modp1=p2+13p+4(1)p14p2α(p)4(1)p14α(p)+4α2(p).

    This proves Lemma 3.

    Lemma 4. Let p be a prime with p1mod4. Then, we have the identities

    p1a=0p1b=0p1c=0a4+b4c4+1modp(a2+b2c21p)=4p1a=0p1b=0p1c=0a2+b2c2+1modp(ab(a+bc1)p)+O(p).

    Proof. Let

    S=p1a=0p1b=0p1c=0a2+b2c2+1modp(a+bc1p).

    The proof of the lemma is divided into the following four parts:

    (ⅰ) There is no Legendre symbol after S. From a complete residue system modulo p, we have

    p1a=0p1b=0p1c=0a2+b2c2+1modp(a+bc1p)=p1a=0p1b=0p1c=0(a+c)2+(b+1)2c2+1modp(a+bp)=p1a=0p1b=0p1c=0a(a+2c)+b2+2b0modp(a+bp)=p1a=0p1b=0p1c=0ac+b2+2b0modp(a+bp)=p1c=0p1b=0b2+2b0modp(bp)+p1a=1p1b=0p1c=0c+b2+2b0modp(a+bp)=(2p)p+p1a=1p1b=0(a+bp)=(2p)p. (2.12)

    (ⅱ) Legendre symbol contains one variable after S. Then, we can get

    p1a=0p1b=0p1c=0a2+b2c2+1modp(a+bc1p)(bp)=p1a=0p1b=0p1c=0a2+b2c2+1modp(a+bc1p)(ap)=p1a=0p1b=0p1c=0a2+b(b+2c)1modp(a+b1p)(ap)=p1a=0p1b=0p1c=0a2+bc1modp(a+b1p)(ap)=p1a=0p1c=0a21modp(a1p)(ap)+p1a=0p1b=1p1c=0a2+c1modp(a+b1p)(ap)=(2p)p+p1a=0p1b=1(a+b1p)(ap)=(2p)p+1. (2.13)

    From (2.11) we have

    p1a=0p1b=0p1c=0a2+b2c2+1modp(a+bc1p)(cp)=p1a=0p1b=0p1c=1a2c2+b2c2c2+1modp(ac+bcc1p)(cp)=p1a=0p1b=0p1c=1a2+b21+¯c2modp(a+b1¯cp)=(2p)pp1a=0p1b=0a2+b21modp(a+b1p)=(2p)pp1a=0p1b=0a2+b2+2b0modp(a+bp)=(2p)pp1a=0p1b=1a2+1+2¯b0modp(a+1p)(bp)=(2p)p(2p)p1a=0p1b=1a2+1+b0modp(a+1p)(bp)=(2p)p(2p)p1a=0(a+1p)(a2+1p)=(2p)p(2p)p1a=1(ap)(a22a+2p)=(2p)p(2p)p1a=1(2a2+¯ap). (2.14)

    (ⅲ) Legendre symbol contains one variable after S. Then, we can get

    p1a=0p1b=0p1c=0a2+b2c2+1modp(a+bc1p)(abp)=p1a=0p1b=1p1c=0a2b2+b2c2b2+1modp(ab+bcb1p)(ap)=p1a=0p1b=1p1c=0a2+1c2+¯b2modp(a+1c¯bp)(abp)=p1a=0p1b=0p1c=0a2+b2c2+1modp(a+bc1p)(acp)=p1a=0p1b=0p1c=0a2+b2c2+1modp(a+bc1p)(bcp). (2.15)

    (ⅳ) Legendre symbol contains one variable after S. Then, we can get

    p1a=0p1b=0p1c=0a2+b2c2+1modp(a+bc1p)(abcp)=p1a=0p1b=0p1c=1a2c2+b2c2c2+1modp(ac+bcc1p)(abc3p)=p1a=0p1b=0p1c=1a2+b21+¯c2modp(a+b1¯cp)(abp)=p1a=0p1b=0p1c=0a2+b2c2+1modp(a+bc1p)(abp)p1a=1p1b=1a2+b21modp(a+b1p)(abp)=p1a=0p1b=0p1c=0a2+b2c2+1modp(a+bc1p)(abp)+O(p). (2.16)

    From (2.12)–(2.16) and the properties of the Legendre symbol modulo p, we have

    p1a=0p1b=0p1c=0a4+b4c4+1modp(a2+b2c21p)=p1a=0p1b=0p1c=0a2+b2c2+1modp(a+bc1p)(1+(ap))(1+(bp))(1+(cp))=4p1a=0p1b=0p1c=0a2+b2c2+1modp(ab(a+bc1)p)+O(p).

    This proves Lemma 4.

    Now, we apply Lemmas 1–4 in Section 2 to complete the proofs of our theorems. For any positive integer q>1 and integer n, note the trigonometric identities

    qa=0e(naq)={qif qn;0if qn. (3.1)

    If (n,p)=1, then we have

    p1a=0e(na2p)=1+p1a=1(1+χ2(a))e(nap)=χ2(n)τ(χ2), (3.2)

    where χ2=(p) denotes the Legendre symbol modulo p, and τ(χ)=p1a=1χ(a)e(ap) denotes the classical Gauss sums.

    From (3.1), (3.2), and the properties of a reduced residue system modulo p, we have the identities

    S4(p)=p1m=0|p1a=0e(ma4+a2p)|4=p1m=0p1a=0p1b=0p1c=0p1d=0e(m(a4+b4c4d4)+a2+b2c2d2p)=p1a=0p1b=0p1c=0p1d=0p1m=0e(m(a4+b4c4d4)p)e(a2+b2c2d2p)=pp1a=0p1b=0p1c=0p1d=0a4+b4c4+d4modpe(a2+b2c2d2p)=pp1a=0p1b=0p1c=0p1d=1a4+b4c4+1modpe(d2(a2+b2c21)p)+pp1a=0p1b=0p1c=0a4+b4c4modpe(a2+b2c2p)=pp1a=0p1b=0p1c=0a4+b4c4+1modpp1d=0e(d2(a2+b2c21)p)+pp1a=0p1b=0p1c=0a4+b4c4modpe(a2+b2c2p)pp1a=0p1b=0p1c=0a4+b4c4+1modp1=p2p1a=0p1b=0p1c=0a4+b4c4+1modpa2+b2c2+1modp1+pτ(χ2)p1a=0p1b=0p1c=0a4+b4c4+1modp(a2+b2c21p)+pp1a=0p1b=1p1c=0a4+1c4modpe(b2(a2+1c2)p)pp1a=0p1b=0p1c=0a4+b4c4+1modp1+pp1a=0p1c=0a4c4modpe(a2c2p)=p2p1a=0p1b=0p1c=0a4+b4c4+1modpa2+b2c2+1modp1+pτ(χ2)p1a=0p1b=0p1c=0a4+b4c4+1modp(a2+b2c21p)+p2p1a=0p1c=0a4+1c4modpa2+1c2modp1+pτ(χ2)p1a=0p1c=0a4+1c4modp(a2+1c2p)pp1a=0p1c=0a4+1c4modp1pp1a=0p1b=0p1c=0a4+b4c4+1modp1+pp1a=0p1c=0a4c4modpe(a2c2p). (3.3)

    Now, we prove Theorem 1. If p3mod4, then S4(p) is a real number, τ(χ2)=ip (see Theorem 9.13 in [1]) is a pure imaginary number, and

    p1a=0p1c=0a4c4modpe(a2c2p)=1+p1a=1a41modpp1c=1e(c2(a21)p)=1+2(p1)=2p1. (3.4)

    So, the sum of the coefficients of τ(χ2) in (23) must be zero. That is,

    p1a=0p1b=0p1c=0a4+b4c4+1modp(a2+b2c21p)+p1a=0p1c=0a4+1c4modp(a2+1c2p)=0. (3.5)

    Combining (3.3)–(3.5), Lemma 1 and Lemma 2, we have

    S4(p)=p1m=0|p1a=0e(ma4+a2p)|4=4p2(2p3)+2p2p(p1)p(p2+p)+p(2p1)=p2(7p10).

    This proves Theorem 1.

    Theorem 2 and some notes follows from (3.3), Lemma 3 and Lemma 4.

    This completes the proofs of all our results.

    The main result of this paper is to give an exact calculating formula for the fourth power mean of one special two-term exponential sum. That is,

    S4(p)=p1m=0|p1a=0e(ma4+a2p)|4=p2(7p10)

    with the case p3mod4. If p1mod4, then we cannot get any non-trivial results for S4(p) yet. We also point out the key to the problem, which is we do not know the exact value of

    p1a=0p1b=0p1c=0a4+b4c4+1modp(a2+b2c21p) (4.1)

    and do not know a valid asymptotic formula for it. However, we get some periodic results. At the same time, some problems to be further studied are also proposed.

    In any case, our work provides a new method for the study of relevant problems. We have a reason to believe that this work will play a positive role in promoting the study of relevant problems.

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

    The authors would like to thank the reviewers for their very helpful and detailed comments, which have significantly improved the presentation of this paper. This work is supported by the National Natural Science Foundation of China (12126357), and the Natural Science Foundation of Shannxi Province (2022JM-017, 2023-JC-YB-013).

    The authors declare that there are no conflicts of interest regarding the publication of this paper.



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