Home Error term of the mean value theorem for binary Egyptian fractions
Article Open Access

Error term of the mean value theorem for binary Egyptian fractions

  • Xuanxuan Xiao EMAIL logo and Wenguang Zhai
Published/Copyright: November 19, 2020

Abstract

In this article, the error term of the mean value theorem for binary Egyptian fractions is studied. An error term of prime number theorem type is obtained unconditionally. Under Riemann hypothesis, a power saving can be obtained. The mean value in short interval is also considered.

MSC 2010: 11F66; 11F67; 11F72

1 Introduction

Let a , n + and ( a , n ) = 1 . Egyptian fractions concern the representation of rational numbers as the finite sum of distinct unit fractions:

a n = 1 x 1 + 1 x 2 + + 1 x k ,

with positive integers x 1 , x 2 , , x k . The problem has a long history and has attracted interests of many authors. For k = 3 , the famous Erdös-Straus conjecture [1] states that the Diophantine equation

4 n = 1 x 1 + 1 x 2 + 1 x 3

is always soluble. This conjecture is still open, although much work has been carried out. See [2,3,4], for example, for more details about the ternary conjecture. Refer to [5] for more information on Egyptian fractions.

Considering the binary Egyptian fractions when k = 2 , define

R ( n ; a ) = card ( x , y ) 2 : a n = 1 x + 1 y .

The Diophantine equation is not always necessary to have a solution. For example, for n with all its prime factor p of the form p 1 ( mod a ) , it has no such representation. Thus, it is natural to consider the mean value of R ( n ; a ) . For X > 0 , define

S ( X ; a ) = n X ( n , a ) = 1 R ( n ; a ) .

Huang and Vaughan [6] proved that

(1) S ( X ; a ) = D ( X ; a ) + Δ ( X ; a ) ,

with

(2) D ( X ; a ) = 3 π 2 a p | a p 1 p + 1 X ( log X ) 2 + C 1 ( a ) log X + C 0 ( a )

and

(3) Δ ( X ; a ) a ϕ ( a ) X 1 / 2 ( log X ) 5 p | a ( 1 p 1 / 2 ) 1 ,

where

C 1 ( a ) = 6 γ 4 ζ ( 2 ) ζ ( 2 ) 2 + p | a 6 p + 2 p 2 1 log p

and

C 0 ( a ) = 2 ( log a ) 2 4 ( log a ) p | a log p p 1 + O ( a ϕ 1 ( a ) log a ) .

Here ζ ( s ) denotes the Riemann zeta function. In [7], Jia got a more explicit expression with better error term for C 0 ( a ) . See [8,9,10] for more results about R ( n ; a ) .

In [6], Huang and Vaughan employed for the first time in this area, of complex analytic technique from multiplicative number theory, and gave an innovative counting function with a different criterion with Croot et al. in [11]. Their estimate (3) holds uniformly for X and a and the error term is almost optimal. The bound for the error here is as strong as can be established on generalized Riemann hypothesis (GRH) with their method. The aim of this paper is to improve the estimate (3) concerning X.

Theorem 1

Let X > 0 and Δ ( X ; a ) be defined in (1). We have

Δ ( X ; a ) a 2 α + ε X 1 / 2 exp { c ( log X ) 3 / 5 ( log log X ) 1 / 5 } ,

with

α = 1864 / 5073 = 0.36744

and some absolute constant c > 0 . Here the implied constant depends only on ε .

Remark 1

Theorem 1 is better than (3) when a is small. Obviously, Theorem 1 is a PNT (prime number theorem) type result, which depends on the zero-free region of the Riemann zeta-function. So in some sense, it is the best possible result under the present methods in the analytic number theory. It is impossible to improve the exponent 1/2 in Theorem 1 without better zero-free region of the Riemann zeta-function.

Under Riemann hypothesis (RH), we can prove the following power saving result.

Theorem 2

Let X > 0 and Δ ( X ; a ) be defined in (1). Assuming RH, we have

Δ ( X ; a ) a 2 α + ε X ( 1 β ) / ( 3 4 β ) ,

with α as above and

β = 2498 / 5073 = 0.4924108 .

Here the implied constant depends only on ε .

Remark 2

One main tool in [6] is the well-known Perron formula. Our proof relies on the convolution method, the results concerning divisor problems with Dirichlet characters (see [12,13]) and moment results of the Dirichlet L-functions.

In the authors’ another work [14], the mean square of the error term under RH was studied. An asymptotic formula can be obtained, which suggests that the average size of the error term is O a ( X 1 / 3 + ε ) .

Both Theorems 1 and 2 depend on zeros of ζ ( s ) . To avoid this point, it is interesting to consider the average value in short intervals. For X , Y > 0 , we define

S ( X , Y ; a ) = X n X + Y ( n , a ) = 1 R ( n ; a ) .

Then we can get the following estimate.

Theorem 3

Let ε > 0 , X > a 90 and X β + ε Y X . We have

S ( X , Y ; a ) = D ( X + Y ; a ) D ( X ; a ) + O a ε Y X ε + a 2 α + ε X β + ε ,

with same α and β as above, where D ( ; a ) is defined by (2).

Remark 3

For the proof of Theorem 3, we use the technique of Zhai [15] who considered the short interval distribution of a class of integers, and his lemma (see Lemma 8) can help us to get some saving in short interval. The constraint for X > a 90 is needed for the character sum (see Lemma 2). We can also use Lemma 1 to get a slightly worse result if it is removed from the theorem.

In what follows, c 1 , c 2 , and C 1 , C 2 , C 3 , denote absolute positive constants. Denote by ε small positive constant which may take different values at each occurrence. For s , we denote s = σ + i t .

2 Preliminary

In this section, we list some lemmas which will be needed in the proof.

We cite a theorem of Friedlander and Iwaniec [12].

Lemma 1

Let χ j ( mod q j ) , j = 1 , 2 , 3 be primitive characters and denote Q = q 1 q 2 q 3 . For any u 1 , we have

n 1 n 2 n 3 u χ 1 ( n 1 ) χ 2 ( n 2 ) χ 3 ( n 3 ) = M 1 ( u ) + O ( Q 2 α 0 u β 0 + ε ) ,

with α 0 = 38 / 75 and β 0 = 37 / 75 , where the main term is given by

M 1 ( u ) = Res s = 1 L ( s , χ 1 ) L ( s , χ 2 ) L ( s , χ 3 ) u s / s ,

and the implied constant depends only on ε .

For primitive character χ ( mod q ) , define by

(4) n = 1 d 3 ( n ; χ ) n s = ζ ( s ) L ( s , χ ) L ( s , χ ¯ ) ,

whence we get

d 3 ( n ; χ ) = n = n 1 n 2 n 3 χ ( n 2 ) χ ¯ ( n 3 )

and

d 3 ( n ; χ ) d 3 ( n ) .

Also for χ = χ 0 ,

d 3 ( n ; χ 0 ) = d 3 ( n ) .

The following lemma is due to Nowak [13], which has more precise estimation than the theorem given by Friedlander and Iwaniec for the special case given below.

Lemma 2

Let q > 1 . Let χ ( mod q ) be a primitive character. For any u q 2 and λ 2 log q log u , we have

n u d 3 ( n ; χ ) = M 2 ( u ) + Δ 0 ( u ; χ ) ,

with

Δ 0 ( u ; χ ) q 2 α u β + ε

and

( α , β ) 1864 5073 , 2498 5073 , 0 < λ λ 0 = 2852 25487 = 0.1119 , 4672 12387 , 6086 12387 , 2852 25487 < λ 1 .

Here the main term is given by

M 2 ( u ) = | L ( 1 , χ ) | 2 u ,

and the implied constant depends only on ε .

Lemma 3

For any u 1 , we have

n u d 3 ( n ) = M 3 ( u ) + O ( u 43 / 96 + ε ) ,

with the implied constant depending only on ε . Here the main term is given by

M 3 ( u ) = Res s = 1 ζ 3 ( s ) u s / s = u P 2 ( log u ) ,

where P 2 ( ) is a polynomial of degree 2.

For y > 0 , define

(5) f y ( s ) = n > y μ ( n ) n s .

Then we have

Lemma 4

Assuming RH, then we have

f y ( s ) y 1 / 2 σ + ε ( 1 + | t | ) ε , 1 / 2 + ε < Re s 1 .

Proof

Well-known.□

The estimation for the mean value of the Möbius function depends on the zero-free region of Riemann zeta function (see for example Theorem 12.7 [16]).

Lemma 5

Let u > 0 . There is an absolute constant c 1 > 0 such that

(6) n u μ ( n ) u exp { c 1 ( log u ) 3 / 5 ( log log u ) 1 / 5 } .

The following results about moments of zeta function and Dirichlet L-functions are well-known (see [17] and Theorem 10.1 of [18]).

Lemma 6

Let T 2 , then we have

T T ζ 1 2 + i t 2 d t T log T

and

χ ( mod a ) T T L 1 2 + i t , χ 4 d t ϕ ( a ) T ( log ( a T ) ) 4 ,

where indicates that the sum is over the primitive characters modulo a.

Lemma 7

Let T 2 , then

χ ( mod a ) T T L 1 2 + i t , χ 4 d t a T ( log ( a T ) ) 4 ,

where χ is the primitive character inducing χ .

Proof

Let χ modulo q be a primitive character. Then we have

χ ( mod a ) T T L 1 2 + i t , χ 4 d t = q | a χ ( mod q ) T T L 1 2 + i t , χ 4 d t .

Then according to Lemma 6, we get

χ ( mod a ) T T 1 2 + i t , χ 4 d t T ( log ( a T ) ) 4 q | a ϕ ( q ) = a T ( log ( a T ) ) 4 .

The following lemma is due to [15], which gives an upper bound for some summation in short intervals.

Lemma 8

Let x > 0 and x 1 / 5 + ε y x . Then

x < m 2 < x + y > x ε 1 y x ε + x 1 / 5 log x .

3 Proof of Theorem 1

First of all, we assume that

(7) ( log X ) 3 / 5 ( log log X ) 1 / 5 log a .

Otherwise, the theorem follows from the upper bound (3).

We start from the identity (see (3.1) in [6])

(8) S ( X ; a ) = 1 ϕ ( a ) χ ( mod a ) χ ¯ ( 1 ) n X D χ ( n ) ,

where

D χ ( n ) = χ ¯ ( n ) u | n 2 χ ( u ) .

For Re s > 1 , define

F χ ( s ) n = 1 D χ ( n ) n s .

Then F χ ( s ) can be written as the form (see (3.2) in [6])

F χ ( s ) = L ( s , χ 0 ) L ( 2 s , χ 0 ) L ( s , χ ) L ( s , χ ¯ ) , Re s > 1 ,

where χ 0 is the principal character modulo a and F χ ( s ) can be analytically continued to .

If χ is a non-principal character modulo q ( χ is the primitive character induced from χ ), we have

F χ ( s ) = L ( s , χ 0 ) L ( 2 s , χ 0 ) L ( s , χ ) L ( s , χ ¯ ) = ζ ( s ) ζ ( 2 s ) L ( s , χ ) L s , χ ¯ p | a ( 1 p s ) 1 χ ( p ) p s 1 χ ¯ ( p ) p s p | a ( 1 p 2 s ) ζ ( s ) ζ ( 2 s ) L ( s , χ ) L s , χ ¯ n = 1 h 1 ( n ; χ ) n s .

If χ = χ 0 , we have

F χ ( s ) = L 3 ( s , χ 0 ) L ( 2 s , χ 0 ) = ζ ( s ) 3 ζ ( 2 s ) p | a ( 1 p s ) 3 p | a ( 1 p 2 s ) ζ ( s ) 3 ζ ( 2 s ) n = 1 h 2 ( n ; χ 0 ) n s .

Noting that h i ( n , χ ) , i = 1 , 2 , is supported on n | a and the series

n = 1 h i ( n , χ ) n s

converges absolutely for σ > 0 , we have

(9) n u | h i ( n , χ ) | ( a u ) ε , u > 0 .

Hence, we can write

(10) n X D χ ( n ) = n 3 X h ( n 3 ; χ ) I X n 3 ; χ ,

where

h ( ; χ ) h 1 ( ; χ ) , χ χ 0 , h 2 ( ; χ ) , χ = χ 0 ,

and for T > 2 and primitive character χ modulo q | a

(11) I ( T ; χ ) n 1 n 2 2 T d 3 ( n 1 ; χ ) μ ( n 2 )

with d 3 ( ; χ ) being defined by (4).

Proposition 1

Let T a 4 and χ χ 0 . We have

(12) I ( T ; χ ) = 6 π 2 T | L ( 1 , χ ) | 2 + O a 2 α T 1 / 2 exp c 2 ( log T ) 3 / 5 ( log log T ) 1 / 5 .

Proof

When χ χ 0 , we write the sum (11) as

I ( T ; χ ) = n 1 z d 3 ( n 1 ; χ ) n 2 ( T / n 1 ) 1 / 2 μ ( n 2 ) + n 2 ( T / z ) 1 / 2 μ ( n 2 ) n 1 T / n 2 2 d 3 ( n 1 ; χ ) n 2 ( T / z ) 1 / 2 μ ( n 2 ) n 1 z d 3 ( n 1 ; χ ) 1 + 2 3 ,

where a 2 z < T is a parameter to be determined.

For the first sum, by using (6) and Lemma 3, we get

1 n 1 z d 3 ( n 1 ) T n 1 exp c 1 log T n 1 3 / 5 log log T n 1 1 / 5 T 1 / 2 exp c 3 ( log T ) 3 / 5 ( log log T ) 1 / 5 n 1 z d 3 ( n 1 ) n 1 1 / 2 T 1 / 2 exp c 3 ( log T ) 3 / 5 ( log log T ) 1 / 5 z 1 / 2 log 2 z .

Similarly, we have

3 T z exp c 1 log T z 3 / 5 log log T z 1 / 5 z log 2 z T 1 / 2 exp c 4 ( log T ) 3 / 5 ( log log T ) 1 / 5 z 1 / 2 log 2 z .

Since T a 4 , as a consequence of Lemma 2, we have

(13) 2 = n 2 ( T / z ) 1 / 2 μ ( n 2 ) M T / n 2 2 + O a 2 α T / n 2 2 β + ε = 21 + O a 2 α T 1 / 2 z 1 / 2 + β + ε ,

with

21 = n 2 ( T / z ) 1 / 2 μ ( n 2 ) Res s = 1 ζ ( s ) L s , χ L s , χ ¯ T / n 2 2 s / s .

Then, for χ χ 0 , we have by using (6)

21 = n 2 ( T / z ) 1 / 2 μ ( n 2 ) | L ( 1 , χ ) | 2 ( T / n 2 2 ) = T | L ( 1 , χ ) | 2 n 2 ( T / z ) 1 / 2 μ ( n 2 ) n 2 2 = T | L ( 1 , χ ) | 2 ζ ( 2 ) 1 + O T 1 / 2 | L ( 1 , χ ) | 2 z 1 / 2 exp c 5 ( log T ) 3 / 5 ( log log T ) 1 / 5 .

Taking

z = exp c 0 ( log T ) 3 / 5 ( log log T ) 1 / 5

for some sufficiently small c 0 > 0 , we can get the result.□

Remark 4

If we remove the constraint T > a 4 , we can employ Lemma 1 instead of Lemma 2 in (13). Then the power 2 α of a will be replaced by 2 α 0 .

Proposition 2

Let T > 0 . We have

(14) I ( T ; χ 0 ) = T n 2 μ ( n 2 ) n 2 2 1 2 log T n 2 2 2 + C 1 log T n 2 2 + C 2 + O T 1 / 2 exp c 6 ( log T ) 3 / 5 ( log log T ) 1 / 5 .

Proof

We can apply similar argument to the proof above and get

I ( T ; χ 0 ) = D ( T , z ) + O T 1 / 2 z 1 / 2 + ε exp c 7 ( log T ) 3 / 5 ( log log T ) 1 / 5 ,

with

D ( T , z ) = n 2 ( T / z ) 1 / 2 μ ( n 2 ) Res s = 1 ζ 3 ( s ) ( T / n 2 2 ) s s = T n 2 ( T / z ) 1 / 2 μ ( n 2 ) n 2 2 1 2 log T n 2 2 2 + C 1 log T n 2 2 + C 2 ,

where C 1 and C 2 are absolute constants. By using (6) again, we have

D ( T , z ) = T n 2 μ ( n 2 ) n 2 1 2 log T n 2 2 2 + C 1 log T n 2 2 + C 2 + O T 1 / 2 z 1 / 2 exp c 8 ( log T ) 3 / 5 ( log log T ) 1 / 5 ,

which implies (14) by taking z as the proof in Proposition 1.□

By an appeal to (8), (10) and (12), we have

(15) S 1 ( X ; a ) 1 ϕ ( a ) χ ( mod a ) χ χ 0 χ ¯ ( 1 ) n 3 X h ( n 3 ; χ ) I X n 3 ; χ = 1 ( X , a ) + 1 ( X , a ) ,

with

1 ( X , a ) = 6 π 2 X ϕ ( a ) χ ( mod a ) χ χ 0 χ ¯ ( 1 ) | L ( 1 , χ ) | 2 n 3 X h ( n 3 ; χ ) n 3

and

1 a 2 α ϕ ( a ) X 1 / 2 χ ( mod a ) χ χ 0 | χ ¯ ( 1 ) | n 3 X / a 20 | h ( n 3 ; χ ) | n 3 1 / 2 exp c 2 log X n 3 3 / 5 log log X n 3 1 / 5 + a 2 α 0 ϕ ( a ) X 1 / 2 χ ( mod a ) χ χ 0 | χ ¯ ( 1 ) | n 3 > X / a 20 | h ( n 3 ; χ ) | n 3 1 / 2 exp c 2 log X n 3 3 / 5 log log X n 3 1 / 5 .

Thanks to (7) and (9), the first term on the right is

a 2 α + ε X 1 / 2 exp c 9 ( log X ) 3 / 5 ( log log X ) 1 / 5

and the second term on the right is

a 10 + 2 α 0 + ε X ε .

Therefore, we have

(16) 1 ( X , a ) a 2 α + ε X 1 / 2 exp c 9 ( log X ) 3 / 5 ( log log X ) 1 / 5 .

For the main term,

(17) 1 ( X , a ) = 6 π 2 p | a p p + 1 X ϕ ( a ) χ ( mod a ) χ χ 0 χ ¯ ( 1 ) | L ( 1 , χ ) | 2 + O ( ( a X ) ε ) .

Therefore, we obtain

(18) S 1 ( X ; a ) = 6 π 2 p | a p p + 1 X ϕ ( a ) χ ( mod a ) χ χ 0 χ ¯ ( 1 ) | L ( 1 , χ ) | 2 + O a 2 α + ε X 1 / 2 exp c 9 ( log X ) 3 / 5 ( log log X ) 1 / 5 .

By an appeal to (8), (10) and (14), we have

(19) S 2 ( X ; a ) 1 ϕ ( a ) n 3 X h ( n 3 ; χ 0 ) I X n 3 ; χ 0 = 2 ( X , a ) + 2 ( X , a ) ,

where

(20) 2 ( X , a ) = X ϕ ( a ) n 3 h ( n 3 ; χ ) n 3 n 2 μ ( n 2 ) n 2 2 1 2 log X n 2 2 n 3 2 + C 1 log X n 2 2 n 3 + C 2 + R ( X )

with

R ( X ) a ε ϕ ( a ) X ε

and

2 ( X , a ) a ε ϕ ( a ) X 1 / 2 exp c 10 ( log X ) 3 / 5 ( log log X ) 1 / 5 .

It is easy to check that the main term in (20) equals to

1 ϕ ( a ) Res s = 1 ζ 3 ( s ) ζ ( 2 s ) n h ( n , χ ) n s X s s .

Therefore, we obtain

(21) S 2 ( X ; a ) = 1 ϕ ( a ) Res s = 1 ζ 3 ( s ) ζ ( 2 s ) p | a ( p s 1 ) 2 p s ( p s + 1 ) X s s + O a ε X 1 / 2 ϕ ( a ) exp c 10 ( log X ) 3 / 5 ( log log X ) 1 / 5 .

Combining (18) and (21), and according to the computation of Huang and Vaughan in [6] about the residue, we get

S ( X ; a ) = C a X ( log X ) 2 + C 1 ( a ) log X + C 0 ( a ) + O a 2 α + ε X 1 / 2 exp c ( log X ) 3 / 5 ( log log X ) 1 / 5 ,

where C a , C 1 ( a ) and C 0 ( a ) are defined in (1).

4 Proof of Theorem 2

It is easy to get the upper bound from (3) when X a 99 . So we assume

X a 99 .

W start from (11). Let 1 < y X 1 / 2 be a parameter to be chosen. We write the sum as

(22) I ( T ; χ ) = n 2 y μ ( n 2 ) n 1 T n 2 2 d 3 ( n 1 ; χ ) + n 2 > y μ ( n 2 ) n 1 T n 2 2 d 3 ( n 1 ; χ ) S 1 + S 2 .

We write according to Lemmas 2 and 3

n 1 T n 2 2 d 3 ( n 1 ; χ ) = M T n 2 2 ; χ + Δ 0 T n 2 2 ; χ ,

where

M ( u ; χ ) = Res s = 1 ζ ( s ) L ( s , χ ) L ( s , χ ¯ ) u s / s ,

and for u a 2

(23) Δ 0 ( u ) = Δ 0 ( u ; χ ) a 2 α u β + ε , χ χ 0 , u 43 / 96 + ε , χ = χ 0 .

Then

(24) S 1 = n 2 y μ ( n 2 ) M T n 2 2 ; χ + n 2 y μ ( n 2 ) Δ 0 T n 2 2 ; χ n 2 y μ ( n 2 ) M T n 2 2 ; χ + S 1 ( y , T , χ ) .

By (23) and Lemma 2 (here the exponent 18 in the following is chosen to make sure that λ < λ 0 ), for χ χ 0 ,

(25) S 1 ( y , T , χ ) a 2 α T β + ε y 1 2 β + ε , y T 1 / 2 / a 18 , a 2 α 0 T β 0 + ε y 1 2 β 0 + ε , y T 1 / 2 / a 18 ,

and for χ = χ 0

(26) S 1 ( y , T , χ 0 ) T 43 / 96 + ε y 5 / 48 + ε .

It remains to compute S 2 . We first consider the case χ χ 0 . Noting that

n n = n 1 n 2 2 n 2 > y d 3 ( n 1 ; χ ) μ ( n 2 ) n s = ζ ( s ) L ( s , χ ) L ( s , χ ¯ ) f y ( 2 s ) ,

with f y ( s ) defined by (5), as a consequence of Perron’s formula

(27) S 2 = 1 2 π i 1 + 1 log T i T 1 + 1 log T + i T ζ ( s ) L ( s , χ ) L ( s , χ ¯ ) f y ( 2 s ) T s s d s + O T 1 + ε T ,

for T = T 10 .

Move the line of integral in (27) to Re s = 1 / 2 . The residue theorem gives

1 2 π i 1 + 1 log T i T 1 + 1 log T + i T ζ ( s ) L ( s , χ ) L s , χ ¯ f y ( 2 s ) T s s d s = Res s = 1 ζ ( s ) L ( s , χ ) L s , χ ¯ f y ( 2 s ) T s s + I χ ( T ) + I h ( T ) ,

with

(28) I χ ( T ) = 1 2 π i 1 / 2 i T 1 / 2 + i T ζ ( s ) L ( s , χ ) L s , χ ¯ f y ( 2 s ) T s s d s

and

I h ( T ) = 1 2 π i 1 / 2 + i T 1 + 1 log T + i T + 1 + 1 log T i T 1 / 2 i T ζ ( s ) L ( s , χ ) L s , χ ¯ f y ( 2 s ) T s s d s .

Assuming RH, using convexity bound for Dirichlet L-function and Lemma 4, the contribution from the horizontal path is

(29) I h ( T ) a 1 / 2 + ε T 1 / 2 + ε y 1 / 2 + ε T .

Thus, we have

(30) S 2 = Res s = 1 ζ ( s ) L ( s , χ ) L ( s , χ ¯ ) f y ( 2 s ) T s s + I χ ( T ) + I h ( T ) + O ( T 9 + ε ) .

Combining (22), (24), (25), (29) and (30), we can get for χ χ 0

I ( T ; χ ) = n 1 n 2 2 T d 3 ( n 1 ; χ ) μ ( n 2 ) = Res s = 1 ζ ( s ) L ( s , χ ) L ( s , χ ¯ ) n 2 y μ ( n 2 ) T s n 2 s 1 s + Res s = 1 ζ ( s ) L ( s , χ ) L ( s , χ ¯ ) n 2 > y μ ( n 2 ) T s n 2 s 1 s + I χ ( T ) + 1 ( y , T ) ,

with I χ ( T ) defined by (28) and

(31) 1 ( y , T ) a 2 α T β + ε y 1 2 β + ε , y T 1 / 2 / a 18 , a 2 α 0 T β 0 + ε y 1 2 β 0 + ε , y > T 1 / 2 / a 18 .

It implies

(32) n 1 n 2 2 T d 3 ( n 1 ; χ ) μ ( n 2 ) = Res s = 1 ζ ( s ) L ( s , χ ) L ( s , χ ¯ ) ζ ( 2 s ) T s s + I χ ( T ) + 1 ( y , T ) .

Similarly, we can get for χ = χ 0

(33) n 1 n 2 2 T d 3 ( n 1 ) μ ( n 2 ) = Res s = 1 ζ 3 ( s ) ζ ( 2 s ) T s s + I χ 0 ( T ) + 2 ( y , T ) ,

with

(34) I χ 0 ( T ) = 1 2 π i 1 / 2 i T 1 / 2 + i T ζ 3 ( s ) f y ( 2 s ) T s s d s

and

2 ( y , T ) T 43 / 96 + ε y 5 / 48 + ε ,

with the help of (26).

Insert (32) and (33) into (10) and take T = X / n 3 . We get for χ χ 0

n X D χ ( n ) = n 3 X h ( n 3 ; χ ) Res s = 1 ζ ( s ) L ( s , χ ) L ( s , χ ¯ ) ζ ( 2 s ) ( X / n 3 ) s s + I χ X n 3 + 1 y , X n 3 ,

and for χ = χ 0

n X D χ 0 ( n ) = n 3 X h ( n 3 ; χ 0 ) Res s = 1 ζ 3 ( s ) ζ ( 2 s ) ( X / n 3 ) s s + I χ 0 X n 3 + 2 y , X n 3 .

Let S 1 ( X ; a ) be defined by (15). Then

S 1 ( X ; a ) = 1 ϕ ( a ) χ ( mod a ) χ χ 0 χ ¯ ( 1 ) n 3 X h ( n 3 ; χ ) × Res s = 1 ζ ( s ) L ( s , χ ) L ( s , χ ¯ ) ζ ( 2 s ) ( X / n 3 ) s s + I χ X n 3 + 1 y , X n 3 = 1 ( X ; a ) + 1 ( X , a ) + 1 ( X , a ) ,

where 1 ( X ; a ) is the same with (17), say,

1 ( X ; a ) = 6 π 2 p | a p p + 1 X ϕ ( a ) χ ( mod a ) χ χ 0 χ ¯ ( 1 ) | L ( 1 , χ ) | 2 + O ( a ε X ε ) ,

1 ( X ; a ) = 1 ϕ ( a ) χ ( mod a ) χ χ 0 χ ¯ ( 1 ) n 3 X h ( n 3 ; χ ) 1 y , X n 3

and

1 ( X ; a ) = 1 ϕ ( a ) χ ( mod a ) χ χ 0 χ ¯ ( 1 ) n 3 X h ( n 3 ; χ ) I χ X n 3 .

According to (31), we have

1 ( X ; a ) 1 ϕ ( a ) χ ( mod a ) χ χ 0 χ ¯ ( 1 ) n 3 X / a 36 y 2 h ( n 3 ; χ ) 1 y , X n 3 + 1 ϕ ( a ) χ ( mod a ) χ χ 0 χ ¯ ( 1 ) n 3 > X / a 36 y 2 h ( n 3 ; χ ) 1 y , X n 3 .

Thus, we have

1 ( X ; a ) a 2 α X β + ε y 1 2 β + ε + a 2 α 0 + 36 β 0 + ε X ε y 1 + ε .

Thus, under RH, we can improve (18) by

(35) S 1 ( X ; a ) = 6 π 2 p | a p p + 1 X ϕ ( a ) χ ( mod a ) χ χ 0 χ ¯ ( 1 ) | L ( 1 , χ ) | 2 + 1 ( X ; a ) + 1 ( X ; a ) .

Let S 2 ( X ; a ) be defined by (19). Then

S 2 ( X ; a ) = 1 ϕ ( a ) n 3 X h ( n 3 ; χ 0 ) Res s = 1 ζ 3 ( s ) ζ ( 2 s ) ( X / n 3 ) s s + I χ 0 X n 3 + 2 y , X n 3 = 2 ( X ; a ) + 2 ( X ; a ) + 2 ( X ; a ) ,

where 2 ( X ; a ) is the same with (20), say,

2 ( X ; a ) = X ϕ ( a ) n 3 h 1 ( n 3 ; χ 0 ) n 3 n 2 1 2 log X n 2 2 n 3 2 + C 1 log X n 2 2 n 3 + C 2 + O ( a ε X ε )

with

2 ( X ; a ) a ε ϕ ( a ) X 43 / 96 + ε y 5 / 48 + ε

and

2 ( X ; a ) = 1 ϕ ( a ) n 3 X h ( n 3 ; χ 0 ) I χ 0 X n 3 .

Then, under RH, we can improve (21) by

(36) S 2 ( X ; a ) = 1 ϕ ( a ) Res s = 1 ζ 3 ( s ) ζ ( 2 s ) p | a ( p s 1 ) 2 p s ( p s + 1 ) X s s + 2 ( X ; a ) + 2 ( X ; a ) .

In order to estimate 1 ( X ; a ) and 2 ( X ; a ) , we have

1 ( X ; a ) + 2 ( X ; a ) = 1 ϕ ( a ) χ ( mod a ) χ ¯ ( 1 ) n 3 X h ( n 3 ; χ ) I χ X n 3 = 1 ϕ ( a ) χ ( mod a ) χ ¯ ( 1 ) n 3 X h ( n 3 ; χ ) 1 2 π i 1 / 2 i T 1 / 2 + i T ζ ( s ) L ( s , χ ) L s , χ ¯ f y ( 2 s ) ( X / n 3 ) s s d s .

Noting that T = ( X / n 3 ) 10 , Lemma 4 implies that

1 ( X ; a ) + 2 ( X ; a ) y 1 2 + ε a ε ϕ ( a ) X 1 / 2 + ε χ ( mod a ) 2 k T 2 k 1 2 k ζ 1 2 + i t L 1 2 + i t , χ 2 1 | t | d t .

Then Hölder’s inequality indicates

1 ( X ; a ) + 2 ( X ; a ) y 1 2 + ε a ε ϕ ( a ) X 1 / 2 + ε 2 k T 2 k χ ( mod a ) 2 k 1 2 k ζ 1 2 + i t 1 2 + i t , χ 2 d t y 1 2 + ε a ε ϕ ( a ) X 1 / 2 + ε 2 k T 2 k χ 2 k 1 2 k 1 2 + i t 2 d t 1 / 2 χ 2 k 1 2 k L 1 2 + i t , χ 4 d t 1 / 2 .

Therefore, we obtain by Lemmas 6 and 7

(37) 1 ( X ; a ) + 2 ( X ; a ) y 1 2 + ε X 1 / 2 + ε a 1 + ε ϕ ( a ) log a X 4 .

Taking ( α , β ) in Lemma 2 and y = X ( 1 2 β ) / ( 3 4 β ) , combining (35), (36) and (37), we can complete the proof.

5 Mean value in short interval

Appeal to (8), (10) and (11), we can write

S ( X , Y ; a ) = 1 ϕ ( a ) χ ( mod a ) χ ¯ ( 1 ) n 1 X + Y h ( n 1 ; χ ) X n 1 < m 2 < X + Y n 1 μ ( ) d 3 ( m ; χ ) .

Observing that

1 ϕ ( a ) χ ( mod a ) χ ¯ ( 1 ) n 1 > X 3 / 4 h ( n 1 ; χ ) X n 1 < m 2 < X + Y n 1 μ ( ) d 3 ( m ; χ ) 1 ϕ ( a ) χ ( mod a ) n 1 > X 3 / 4 | h ( n 1 ; χ ) | X n 1 < m 2 < X + Y n 1 d 3 ( m ) a ε X 1 / 4 + ε ,

we have

S ( X , Y ; a ) = 1 ϕ ( a ) χ ( mod a ) χ ¯ ( 1 ) n 1 X 3 / 4 h ( n 1 ; χ ) X n 1 < m 2 < X + Y n 1 μ ( ) d 3 ( m ; χ ) + O ( a ε X 1 / 4 + ε ) .

For the cases where characters are non-principal, denote by

P 11 1 ϕ ( a ) χ χ 0 ( mod a ) χ ¯ ( 1 ) n 1 X 3 / 4 h ( n 1 ; χ ) X n 1 < m 2 < X + Y n 1 ( X / n 1 ) ε μ ( ) d 3 ( m ; χ )

and

P 12 1 ϕ ( a ) χ χ 0 ( mod a ) χ ¯ ( 1 ) n 1 X 3 / 4 h ( n 1 ; χ ) X n 1 < m 2 < X + Y n 1 > ( X / n 1 ) ε μ ( ) d 3 ( m ; χ ) .

For principal character case, denote by

P 21 1 ϕ ( a ) n 1 X 3 / 4 h ( n 1 ; χ 0 ) X n 1 < m 2 < X + Y n 1 ( X / n 1 ) ε μ ( ) d 3 ( m )

and

P 22 1 ϕ ( a ) n 1 X 3 / 4 h ( n 1 ; χ 0 ) X n 1 < m 2 < X + Y n 1 > ( X / n 1 ) ε μ ( ) d 3 ( m ) .

Thus, we have

(38) S ( X , Y ; a ) = P 11 + P 12 + P 21 + P 22 + O ( a ε X 1 / 4 + ε ) .

Proposition 3

We have

P 11 = Res s = 1 ζ ( s ) ζ ( 2 s ) χ ( mod a ) χ χ 0 χ ¯ ( 1 ) L ( s , χ ) L s , χ ¯ n = 1 h 1 ( n ; χ ) n s ( X + Y ) s X s s + O X ε Y a ε + a 2 α + ε X β + ε .

Proof

Rewrite P 11 as the form

P 11 = 1 ϕ ( a ) χ χ 0 ( mod a ) χ ¯ ( 1 ) n 1 X 3 / 4 h ( n 1 ; χ ) ( X / n 1 ) ε μ ( ) X n 1 2 < m < X + Y n 1 2 d 3 ( m ; χ ) .

Then according to Lemma 2, for X a 90 , we have

(39) P 11 = 1 ϕ ( a ) χ χ 0 ( mod a ) χ ¯ ( 1 ) n 1 X 3 / 4 h ( n 1 ; χ ) ( X / n 1 ) ε μ ( ) × Y n 1 2 | L ( 1 , χ ) | 2 + O a 2 α X n 1 2 β + ε .

The main term above is

M 11 Y ϕ ( a ) χ χ 0 ( mod a ) χ ¯ ( 1 ) | L ( 1 , χ ) | 2 n 1 X 3 / 4 h ( n 1 ; χ ) n 1 ( X / n 1 ) ε μ ( ) 2 = Y ϕ ( a ) χ χ 0 ( mod a ) χ ¯ ( 1 ) | L ( 1 , χ ) | 2 n 1 X 3 / 4 h ( n 1 ; χ ) n 1 6 π 2 + O X n 1 ε .

Then we can get easily

M 11 = Res s = 1 ζ ( s ) ζ ( 2 s ) χ ( mod a ) χ χ 0 χ ¯ ( 1 ) L ( s , χ ) L ( s , χ ¯ ) n = 1 h 1 ( n ; χ ) n s ( X + Y ) s X s s + O ( a ε X ε Y ) .

The error term in (39) is

E 11 a 2 α + ε X β + ε .

Proposition 4

We have

P 21 = 1 ϕ ( a ) Res s = 1 ζ 3 ( s ) ζ ( 2 s ) n = 1 h 2 ( n ; χ 0 ) n s ( X + Y ) s X s s + O a ε ( Y X ε + X 43 / 96 + ε ) ϕ ( a ) .

Proof

We can write

P 21 = 1 ϕ ( a ) n 1 X 3 / 4 h ( n 1 ; χ 0 ) ( X / n 1 ) ε μ ( ) X n 1 2 < m < X + Y n 1 2 d 3 ( m ) .

Lemma 3 implies

P 21 = 1 ϕ ( a ) n 1 X 3 / 4 h ( n 1 ; χ 0 ) ( X / n 1 ) ε μ ( ) × X + Y n 1 2 P 2 log X + Y n 1 2 X n 1 2 P 2 log X n 1 2 + O X n 1 2 43 / 96 + ε .

Observing that

( X + Y ) P 2 log X + Y n 1 2 X P 2 log X n 1 2 Y log 2 X + log 2 n 1 2 ,

it is easy to check that

P 21 = 1 ϕ ( a ) n 1 X 3 / 4 h n 1 ; χ 0 μ ( ) X + Y n 1 2 P 2 log X + Y n 1 2 X n 1 2 P 2 log X n 1 2 + O a ε ϕ ( a ) 1 Y X ε + X 43 / 96 + ε .

Removing the constraint for n 1 , we can get a smaller error term. Thus,

P 21 = 1 ϕ ( a ) n 1 h ( n 1 ; χ 0 ) μ ( ) X + Y n 1 2 P 2 log X + Y n 1 2 X n 1 2 P 2 log X n 1 2 + O a ε ϕ ( a ) 1 Y X ε + X 43 / 96 + ε ,

which infers

P 21 = 1 ϕ ( a ) Res s = 1 ζ 3 ( s ) ζ ( 2 s ) n = 1 h 2 ( n ; χ 0 ) n s ( X + Y ) s X s s + O a ε Y X ε + X 43 / 96 + ε ϕ ( a ) .

Proposition 5

We have

P 12 a ε X ε 2 ( Y X ε + X 1 / 5 log X )

and

P 22 a ε X ε 2 ϕ ( a ) ( Y X ε + X 1 / 5 log X ) .

Proof

In order to use Lemma 8, we shall cut the length of the summation over n 1 and get

P 12 X ε 2 ϕ ( a ) χ χ 0 ( mod a ) n 1 X 3 / 4 | h ( n 1 ; χ ) | X n 1 < m 2 < X + Y n 1 > ( X / n 1 ) ε 1 + O a ε Y X 1 / 3 + ε .

According to Lemma 8, we get

P 12 X ε 2 ϕ ( a ) χ χ 0 ( mod a ) n 1 X 3 / 4 | h ( n 1 ; χ ) | Y n 1 X n 1 ε + X n 1 1 / 5 log X n 1 + O ( a ε Y X 1 / 3 + ε ) .

Then it is easy to check

P 12 a ε X ε 2 ( Y X ε + X 1 / 5 log X ) .

Similar argument can get the second assertion.□

Combining (38) and Propositions 3–5, we can deduce Theorem 3.

Acknowledgement

Xuanxuan Xiao was supported in part by National Natural Science Foundation of China (11701596) and The Science and Technology Development Fund, Macau SAR (File no. 0095/2018/A3). Wenguang Zhai was supported by National Natural Science Foundation of China (Grant no. 11971476).

References

[1] P. Erdös, AZ 1x1+1x2+⋯+1xn=ab egyenlet egész számú megoldásairól (On a Diophantine equation), Mat. Lapok 1 (1950), 192–210.Search in Google Scholar

[2] C. Elsholtz and T. Tao, Counting the number of solutions to the Erdös-Straus equation on unit fractions, J. Aust. Math. Soc. 94 (2013), no. 1, 50–105.10.1017/S1446788712000468Search in Google Scholar

[3] C. Jia, The estimate for mean values on prime numbers relative to 4p=1n1+1n2+1n3, Sci. China Math. 55 (2012), 465–474.10.1007/s11425-011-4348-9Search in Google Scholar

[4] R. C. Vaughan, On a problem of Erdös, Straus and Schinzel, Mathematika 17 (1970), 193–198.10.1112/S0025579300002886Search in Google Scholar

[5] R. K. Guy, Unsolved Problems in Number Theory, 2nd edition, Springer-Verlag, 1994.10.1007/978-1-4899-3585-4Search in Google Scholar

[6] J. Huang and R. C. Vaughan, Mean value theorems for binary Egyptian fractions, Acta Arith. 155 (2012), 287–296.10.4064/aa155-3-5Search in Google Scholar

[7] C. Jia, Mean value from representation of rational number as sum of two Egyptian fractions, J. Number Theory 132 (2012), 701–713.10.1016/j.jnt.2011.09.007Search in Google Scholar

[8] T. D. Browning and C. Elsholtz, The number of representations of rationals as a sum of unit fractions, Illinois J. Math. 55 (2011) no. 2, 685–696.10.1215/ijm/1359762408Search in Google Scholar

[9] J. Huang and R. C. Vaughan, Mean value theorems for binary Egyptian fractions II, J. Number Theory 131 (2011), 1641–1656.10.4064/aa155-3-5Search in Google Scholar

[10] J. Huang and R. C. Vaughan, On the exceptional set for binary Egyptian fractions, Bull. Lond. Math. Soc. 45 (2013), 861–874.10.1112/blms/bdt020Search in Google Scholar

[11] C. Croot, D. Dobbs, J. Friedlander, A. Hetzel, and F. Pappalardi, Binary Egyptian fractions, J. Number Theory 84 (2000), 63–79.10.1006/jnth.2000.2508Search in Google Scholar

[12] J. Friedlander and H. Iwaniec, Summation formulae for coefficients of L-functions, Canad. J. Math. 57 (2005), no. 3, 494–505.10.4153/CJM-2005-021-5Search in Google Scholar

[13] W. G. Nowak, Refined estimates for exponential sums and a problem concerning the product of three l-series, in: C. Elsholtz, P. Grabner (eds.), Number Theory-Diophantine Problems, Uniform Distribution and Applications, Springer, Cham, 2017, pp. 333–345.10.1007/978-3-319-55357-3_17Search in Google Scholar

[14] X. X. Xiao and W. G. Zhai, Mean square of the error term of the mean value of binary Egyptian fractions, Front. Math. China 15 (2020), no. 1, 183–204.10.1007/s11464-020-0820-6Search in Google Scholar

[15] W. G. Zhai, Short interval results for a class of integers, Monatsh. Math. 140 (2003), 233–257.10.1007/s00605-003-0006-9Search in Google Scholar

[16] A. Ivić, The Riemann Zeta-Functions: Theory and Applications, reprint ed., Dover Publications, 2003.Search in Google Scholar

[17] G. H. Hardy and J. E. Littlewood, Contributions to the theory of the Riemann zeta-function and the theory of the distribution of primes, Acta Math. 41 (1916), no. 1, 119–196.10.1007/BF02422942Search in Google Scholar

[18] H. L. Montgomery, Topics in Multiplicative Number Theory, Springer-Verlag, 1971.10.1007/BFb0060851Search in Google Scholar

Received: 2020-01-24
Revised: 2020-09-17
Accepted: 2020-09-24
Published Online: 2020-11-19

© 2020 Xuanxuan Xiao and Wenguang Zhai, published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

Articles in the same Issue

  1. Regular Articles
  2. Non-occurrence of the Lavrentiev phenomenon for a class of convex nonautonomous Lagrangians
  3. Strong and weak convergence of Ishikawa iterations for best proximity pairs
  4. Curve and surface construction based on the generalized toric-Bernstein basis functions
  5. The non-negative spectrum of a digraph
  6. Bounds on F-index of tricyclic graphs with fixed pendant vertices
  7. Crank-Nicolson orthogonal spline collocation method combined with WSGI difference scheme for the two-dimensional time-fractional diffusion-wave equation
  8. Hardy’s inequalities and integral operators on Herz-Morrey spaces
  9. The 2-pebbling property of squares of paths and Graham’s conjecture
  10. Existence conditions for periodic solutions of second-order neutral delay differential equations with piecewise constant arguments
  11. Orthogonal polynomials for exponential weights x2α(1 – x2)2ρe–2Q(x) on [0, 1)
  12. Rough sets based on fuzzy ideals in distributive lattices
  13. On more general forms of proportional fractional operators
  14. The hyperbolic polygons of type (ϵ, n) and Möbius transformations
  15. Tripled best proximity point in complete metric spaces
  16. Metric completions, the Heine-Borel property, and approachability
  17. Functional identities on upper triangular matrix rings
  18. Uniqueness on entire functions and their nth order exact differences with two shared values
  19. The adaptive finite element method for the Steklov eigenvalue problem in inverse scattering
  20. Existence of a common solution to systems of integral equations via fixed point results
  21. Fixed point results for multivalued mappings of Ćirić type via F-contractions on quasi metric spaces
  22. Some inequalities on the spectral radius of nonnegative tensors
  23. Some results in cone metric spaces with applications in homotopy theory
  24. On the Malcev products of some classes of epigroups, I
  25. Self-injectivity of semigroup algebras
  26. Cauchy matrix and Liouville formula of quaternion impulsive dynamic equations on time scales
  27. On the symmetrized s-divergence
  28. On multivalued Suzuki-type θ-contractions and related applications
  29. Approximation operators based on preconcepts
  30. Two types of hypergeometric degenerate Cauchy numbers
  31. The molecular characterization of anisotropic Herz-type Hardy spaces with two variable exponents
  32. Discussions on the almost 𝒵-contraction
  33. On a predator-prey system interaction under fluctuating water level with nonselective harvesting
  34. On split involutive regular BiHom-Lie superalgebras
  35. Weighted CBMO estimates for commutators of matrix Hausdorff operator on the Heisenberg group
  36. Inverse Sturm-Liouville problem with analytical functions in the boundary condition
  37. The L-ordered L-semihypergroups
  38. Global structure of sign-changing solutions for discrete Dirichlet problems
  39. Analysis of F-contractions in function weighted metric spaces with an application
  40. On finite dual Cayley graphs
  41. Left and right inverse eigenpairs problem with a submatrix constraint for the generalized centrosymmetric matrix
  42. Controllability of fractional stochastic evolution equations with nonlocal conditions and noncompact semigroups
  43. Levinson-type inequalities via new Green functions and Montgomery identity
  44. The core inverse and constrained matrix approximation problem
  45. A pair of equations in unlike powers of primes and powers of 2
  46. Miscellaneous equalities for idempotent matrices with applications
  47. B-maximal commutators, commutators of B-singular integral operators and B-Riesz potentials on B-Morrey spaces
  48. Rate of convergence of uniform transport processes to a Brownian sheet
  49. Curves in the Lorentz-Minkowski plane with curvature depending on their position
  50. Sequential change-point detection in a multinomial logistic regression model
  51. Tiny zero-sum sequences over some special groups
  52. A boundedness result for Marcinkiewicz integral operator
  53. On a functional equation that has the quadratic-multiplicative property
  54. The spectrum generated by s-numbers and pre-quasi normed Orlicz-Cesáro mean sequence spaces
  55. Positive coincidence points for a class of nonlinear operators and their applications to matrix equations
  56. Asymptotic relations for the products of elements of some positive sequences
  57. Jordan {g,h}-derivations on triangular algebras
  58. A systolic inequality with remainder in the real projective plane
  59. A new characterization of L2(p2)
  60. Nonlinear boundary value problems for mixed-type fractional equations and Ulam-Hyers stability
  61. Asymptotic normality and mean consistency of LS estimators in the errors-in-variables model with dependent errors
  62. Some non-commuting solutions of the Yang-Baxter-like matrix equation
  63. General (p,q)-mixed projection bodies
  64. An extension of the method of brackets. Part 2
  65. A new approach in the context of ordered incomplete partial b-metric spaces
  66. Sharper existence and uniqueness results for solutions to fourth-order boundary value problems and elastic beam analysis
  67. Remark on subgroup intersection graph of finite abelian groups
  68. Detectable sensation of a stochastic smoking model
  69. Almost Kenmotsu 3-h-manifolds with transversely Killing-type Ricci operators
  70. Some inequalities for star duality of the radial Blaschke-Minkowski homomorphisms
  71. Results on nonlocal stochastic integro-differential equations driven by a fractional Brownian motion
  72. On surrounding quasi-contractions on non-triangular metric spaces
  73. SEMT valuation and strength of subdivided star of K 1,4
  74. Weak solutions and optimal controls of stochastic fractional reaction-diffusion systems
  75. Gradient estimates for a weighted nonlinear parabolic equation and applications
  76. On the equivalence of three-dimensional differential systems
  77. Free nonunitary Rota-Baxter family algebras and typed leaf-spaced decorated planar rooted forests
  78. The prime and maximal spectra and the reticulation of residuated lattices with applications to De Morgan residuated lattices
  79. Explicit determinantal formula for a class of banded matrices
  80. Dynamics of a diffusive delayed competition and cooperation system
  81. Error term of the mean value theorem for binary Egyptian fractions
  82. The integral part of a nonlinear form with a square, a cube and a biquadrate
  83. Meromorphic solutions of certain nonlinear difference equations
  84. Characterizations for the potential operators on Carleson curves in local generalized Morrey spaces
  85. Some integral curves with a new frame
  86. Meromorphic exact solutions of the (2 + 1)-dimensional generalized Calogero-Bogoyavlenskii-Schiff equation
  87. Towards a homological generalization of the direct summand theorem
  88. A standard form in (some) free fields: How to construct minimal linear representations
  89. On the determination of the number of positive and negative polynomial zeros and their isolation
  90. Perturbation of the one-dimensional time-independent Schrödinger equation with a rectangular potential barrier
  91. Simply connected topological spaces of weighted composition operators
  92. Generalized derivatives and optimization problems for n-dimensional fuzzy-number-valued functions
  93. A study of uniformities on the space of uniformly continuous mappings
  94. The strong nil-cleanness of semigroup rings
  95. On an equivalence between regular ordered Γ-semigroups and regular ordered semigroups
  96. Evolution of the first eigenvalue of the Laplace operator and the p-Laplace operator under a forced mean curvature flow
  97. Noetherian properties in composite generalized power series rings
  98. Inequalities for the generalized trigonometric and hyperbolic functions
  99. Blow-up analyses in nonlocal reaction diffusion equations with time-dependent coefficients under Neumann boundary conditions
  100. A new characterization of a proper type B semigroup
  101. Constructions of pseudorandom binary lattices using cyclotomic classes in finite fields
  102. Estimates of entropy numbers in probabilistic setting
  103. Ramsey numbers of partial order graphs (comparability graphs) and implications in ring theory
  104. S-shaped connected component of positive solutions for second-order discrete Neumann boundary value problems
  105. The logarithmic mean of two convex functionals
  106. A modified Tikhonov regularization method based on Hermite expansion for solving the Cauchy problem of the Laplace equation
  107. Approximation properties of tensor norms and operator ideals for Banach spaces
  108. A multi-power and multi-splitting inner-outer iteration for PageRank computation
  109. The edge-regular complete maps
  110. Ramanujan’s function k(τ)=r(τ)r2(2τ) and its modularity
  111. Finite groups with some weakly pronormal subgroups
  112. A new refinement of Jensen’s inequality with applications in information theory
  113. Skew-symmetric and essentially unitary operators via Berezin symbols
  114. The limit Riemann solutions to nonisentropic Chaplygin Euler equations
  115. On singularities of real algebraic sets and applications to kinematics
  116. Results on analytic functions defined by Laplace-Stieltjes transforms with perfect ϕ-type
  117. New (p, q)-estimates for different types of integral inequalities via (α, m)-convex mappings
  118. Boundary value problems of Hilfer-type fractional integro-differential equations and inclusions with nonlocal integro-multipoint boundary conditions
  119. Boundary layer analysis for a 2-D Keller-Segel model
  120. On some extensions of Gauss’ work and applications
  121. A study on strongly convex hyper S-subposets in hyper S-posets
  122. On the Gevrey ultradifferentiability of weak solutions of an abstract evolution equation with a scalar type spectral operator on the real axis
  123. Special Issue on Graph Theory (GWGT 2019), Part II
  124. On applications of bipartite graph associated with algebraic structures
  125. Further new results on strong resolving partitions for graphs
  126. The second out-neighborhood for local tournaments
  127. On the N-spectrum of oriented graphs
  128. The H-force sets of the graphs satisfying the condition of Ore’s theorem
  129. Bipartite graphs with close domination and k-domination numbers
  130. On the sandpile model of modified wheels II
  131. Connected even factors in k-tree
  132. On triangular matroids induced by n3-configurations
  133. The domination number of round digraphs
  134. Special Issue on Variational/Hemivariational Inequalities
  135. A new blow-up criterion for the Nabc family of Camassa-Holm type equation with both dissipation and dispersion
  136. On the finite approximate controllability for Hilfer fractional evolution systems with nonlocal conditions
  137. On the well-posedness of differential quasi-variational-hemivariational inequalities
  138. An efficient approach for the numerical solution of fifth-order KdV equations
  139. Generalized fractional integral inequalities of Hermite-Hadamard-type for a convex function
  140. Karush-Kuhn-Tucker optimality conditions for a class of robust optimization problems with an interval-valued objective function
  141. An equivalent quasinorm for the Lipschitz space of noncommutative martingales
  142. Optimal control of a viscous generalized θ-type dispersive equation with weak dissipation
  143. Special Issue on Problems, Methods and Applications of Nonlinear analysis
  144. Generalized Picone inequalities and their applications to (p,q)-Laplace equations
  145. Positive solutions for parametric (p(z),q(z))-equations
  146. Revisiting the sub- and super-solution method for the classical radial solutions of the mean curvature equation
  147. (p,Q) systems with critical singular exponential nonlinearities in the Heisenberg group
  148. Quasilinear Dirichlet problems with competing operators and convection
  149. Hyers-Ulam-Rassias stability of (m, n)-Jordan derivations
  150. Special Issue on Evolution Equations, Theory and Applications
  151. Instantaneous blow-up of solutions to the Cauchy problem for the fractional Khokhlov-Zabolotskaya equation
  152. Three classes of decomposable distributions
Downloaded on 9.9.2025 from https://www.degruyterbrill.com/document/doi/10.1515/math-2020-0091/html
Scroll to top button