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A pair of equations in unlike powers of primes and powers of 2

  • Yong Cai and Liqun Hu EMAIL logo
Published/Copyright: July 6, 2020

Abstract

In this article, we show that every pair of large even integers satisfying some necessary conditions can be represented in the form of a pair of one prime, one prime squares, two prime cubes, and 187 powers of 2.

MSC 2010: 11P32; 11P05; 11P55

1 Introduction

As an approximation to Goldbach’s problem, Linnik proved in 1951 [1] under the assumption of the Generalized Riemann Hypothesis (GRH), and later in 1953 [2] unconditionally, that each large even integer N is a sum of two primes p 1 , p 2 and a bounded number of powers of 2, namely

(1.1) N = p 1 + p 2 + 2 ν 1 + + 2 ν k .

In 2002, Heath-Brown and Puchta [3] applied a rather different approach to this problem and showed that k = 13 and, on the GRH, k = 7 . In 2003, Pintz and Ruzsa [4] established this latter result and announced that k = 8 is acceptable unconditionally. Elsholtz, in an unpublished manuscript, which is yet to appear in print, showed that k = 12 ; this was proved independently by Liu and Lü [5].

In 1999, Liu et al. [6] proved that every large even integer N can be written as a sum of four squares of primes and a bounded number of powers of 2, namely

(1.2) N = p 1 2 + p 2 2 + p 3 2 + p 4 2 + 2 v 1 + + 2 v k .

And Platt and Trudgian [7] got that k = 45 suffices.

In 2001, Liu and Liu [8] proved that every large even integer N can be written as a sum of eight cubes of primes and a bounded number of powers of 2, namely

(1.3) N = p 1 3 + p 2 3 + + p 8 3 + 2 v 1 + + 2 v k .

The acceptable value k = 330 was determined by Platt and Trudgian [7].

In 2011, Liu and Lü [9] considered a hybrid problem of (1.1)–(1.3),

(1.4) N = p 1 + p 2 2 + p 3 3 + p 4 3 + 2 v 1 + + 2 v k .

They showed that k = 161 is acceptable and Platt and Trudgian [7] revised it to 156.

As a generalization, recently, Hu and Yang [10] first considered the simultaneous representation of pairs of positive even integers N 2 N 1 > N 2 , in the form

(1.5) N 1 = p 1 + p 2 2 + p 3 3 + p 4 3 + 2 v 1 + + 2 v k , N 2 = p 5 + p 6 2 + p 7 3 + p 8 3 + 2 v 1 + + 2 v k ,

where k is a positive integer. They proved that the simultaneous Eq. (1.5) is solvable for k = 455 .

The primary purpose of this article is to sharpen this result considerably by establishing the following theorem.

Theorem 1.1

For k = 187 , Eq. (1.5) is solvable for every pair of sufficiently large positive even integers N 1 and N 2 satisfying N 2 N 1 > N 2 .

Our proof of Theorem 1.1 uses the Hardy-Littlewood circle method. We make a new estimate of minor arcs and draw on some strategies adopted in the works of Hu and Yang [10] and Kong and Liu [11].

Throughout this article, the letter ϵ denotes a positive constant, which is arbitrarily small but may not the same at different occurrences.

2 The proof of Theorem 1.1

Throughout this article, we assume that N i , i = 1 , 2 are sufficiently large even integers satisfying N 2 N 1 > N 2 . Then, we set

P i = N i 1 / 9 2 ϵ , Q i = N i 8 / 9 + ϵ , L = log 2 N 1

for i = 1 , 2 .

We define the major arcs M 1 , M 2 and minor arcs C ( M 1 ) , C ( M 2 ) as usual, namely

M i = q P i 1 a q ( a , q ) = 1 M i ( a , q ) , C ( M i ) = 1 Q i , 1 + 1 Q i \ M i ,

where i = 1 , 2 and

M i ( a , q ) = α i : α i a q 1 q Q i .

It follows from the definition of P i and Q i that the arcs M 1 ( a , q ) and M 2 ( a , q ) are mutually disjoint, respectively. We further define

M = M 1 × M 2 = ( α 1 , α 2 ) : α 1 M 1 , α 2 M 2 , C ( M ) = 1 Q i , 1 + 1 Q i 2 \ M .

As in [10], let δ = 10 4 and

(2.1) U i = N i 16 ( 1 + δ ) 1 / 3 , V i = U i 5 / 6

for i = 1 , 2 . We set

(2.2) f ( α i , N i ) = p N i ( log p ) e ( p α i ) , g ( α i , N i ) = p N i 1 / 2 ( log p ) e ( p 2 α i ) ,

(2.3) S ( α i , U i ) = p U i ( log p ) e ( p 3 α i ) , T ( α i , V i ) = p V i ( log p ) e ( p 3 α i ) ,

and set

(2.4) G ( α i ) = v L e ( 2 v α i ) , E λ α i [ 0 , 1 ] : G ( α i ) λ L ,

for i = 1 , 2 .

Let

R ( N 1 , N 2 ) = log p 1 log p 2 log p 8

be the weighted number of solutions of (1.5) in ( p 1 , , p 8 , v 1 , , v k ) with

p 1 N 1 , p 2 N 1 1 / 2 , p 3 U 1 , p 4 V 1 , p 5 N 2 , p 6 N 2 1 / 2 , p 7 U 2 , p 8 V 2 , v j L ,

for j = 1 , 2 , , k . Then, R ( N 1 , N 2 ) can be written as follows:

M + C ( M ) E λ + C ( M ) \ E λ f ( α 1 , N 1 ) g ( α 1 , N 1 ) S ( α 1 , U 1 ) T ( α 1 , V 1 ) f ( α 2 , N 2 ) g ( α 2 , N 2 ) S ( α 2 , U 2 ) × T ( α 2 , V 2 ) G k ( α 1 + α 2 ) e ( α 1 N 1 α 2 N 2 ) d α 1 d α 2 R 1 ( N 1 , N 2 ) + R 2 ( N 1 , N 2 ) + R 3 ( N 1 , N 2 ) .

We will establish Theorem 1.1 by estimating the term R 1 ( N 1 , N 2 ) , R 2 ( N 1 , N 2 ) , and R 3 ( N 1 , N 2 ) . We need to show that R ( N 1 , N 2 ) > 0 for every pair of sufficiently large positive even integers N 2 N 1 > N 2 .

Let

C i ( q , a ) = h = 1 q e a h i q

for i = 1 , 2 , 3 , 4 . Then, we write

B ( n , q ) = a = 1 ( a , q ) = 1 q C 1 ( q , a ) C 2 ( q , a ) C 3 ( q , a ) C 3 ( q , a ) e a n q , A ( n , q ) = B ( n , q ) φ 4 ( q ) , S ( n ) = q = 1 A ( n , q ) .

Now, we need to quote two lemmas from Hu and Yang [10, Lemmas 2.3 and 2.4] as follows:

Lemma 2.1

For all integers n 0 ( mod 2 ) , we have S ( n ) 0.2448 .

Lemma 2.2

Let A ( N i , k ) = n i 2 : n i = N i 2 v 1 2 v k with k 2 . Then, for N 1 N 2 0 ( mod 2 ) , we have

n 1 A ( N 1 , k ) n 2 A ( N 2 , k ) n 1 n 2 0 ( mod 2 ) J ( n 1 ) J ( n 2 ) 5.4671 N 1 10 / 9 N 2 10 / 9 L k ,

where J ( n ) is defined as

J ( n ) m 1 + m 2 + m 3 + m 4 = n m 1 N i , m 2 N i , U i 3 < m 3 8 U i 3 , V i 3 < m 4 8 V i 3 m 2 1 / 2 ( m 3 m 4 ) 2 / 3 .

Lemma 2.3

For every pair of sufficiently large positive even integers N 1 and N 2 satisfying N 2 N 1 > N 2 ,

R 1 ( N 1 , N 2 ) 0.00101 N 1 10 / 9 N 2 10 / 9 L k .

Proof

By Hu and Yang [10, Lemma 2.2] we note that

R 1 ( N 1 , N 2 ) = M f ( α 1 , N 1 ) g ( α 1 , N 1 ) S ( α 1 , U 1 ) T ( α 1 , V 1 ) f ( α 2 , N 2 ) g ( α 2 , N 2 ) S ( α 2 , U 2 ) T ( α 2 , V 2 ) × G k ( α 1 + α 2 ) e ( α 1 N 1 α 2 N 2 ) d α 1 d α 2 1 2 3 2 2 n 1 A ( N 1 , k ) n 2 A ( N 2 , k ) S ( n 1 ) S ( n 2 ) J ( n 1 ) J ( n 2 ) .

Then, using Lemmas 2.1 and 2.2 the lemma now follows.□

Lemma 2.4

We have

meas ( E λ ) N 1 E ( λ ) ,

with E ( 0.9322 ) > 845 / 1008 + 10 10 .

Proof

According to Hu and Yang [12, Lemma 5.1], the following lemma can be calculated by computer.□

Lemma 2.5

For every pair of sufficiently large positive even integers N 1 and N 2 satisfying N 2 N 1 > N 2 ,

R 2 ( N 1 , N 2 ) N 1 10 / 9 N 2 10 / 9 L k 1 .

Proof

By the definition of C ( M ) , we have

C ( M ) ( α 1 , α 2 ) : α 1 C ( M 1 ) , α 2 [ 0 , 1 ] ( α 1 , α 2 ) : α 1 [ 0 , 1 ] , α 2 C ( M 2 ) .

Then, R 2 ( N 1 , N 2 ) is

C ( M ) E λ f ( α 1 , N 1 ) g ( α 1 , N 1 ) S ( α 1 , U 1 ) T ( α 1 , V 1 ) f ( α 2 , N 2 ) g ( α 2 , N 2 ) × S ( α 2 , U 2 ) T ( α 2 , V 2 ) G k ( α 1 + α 2 ) e ( α 1 N 1 α 2 N 2 ) d α 1 d α 2 L k ( α 1 , α 2 ) C ( M 1 ) × [ 0 , 1 ] | G ( α 1 + α 2 ) | λ L + ( α 1 , α 2 ) [ 0 , 1 ] × C ( M 2 ) | G ( α 1 + α 2 ) | λ L f ( α 1 , N 1 ) g ( α 1 , N 1 ) × S ( α 1 , U 1 ) T ( α 1 , V 1 ) f ( α 2 , N 2 ) g ( α 2 , N 2 ) S ( α 2 , U 2 ) T ( α 2 , V 2 ) d α 1 d α 2 L k 1 + 2 ,

where we use the trivial bound of G ( α 1 + α 2 ) . We note that

1 ( α 1 , α 2 ) C ( M 1 ) × [ 0 , 1 ] | G ( α 1 + α 2 ) | λ L f ( α 1 , N 1 ) g ( α 1 , N 1 ) S ( α 1 , U 1 ) T ( α 1 , V 1 ) f ( α 2 , N 2 ) g ( α 2 , N 2 ) S ( α 2 , U 2 ) T ( α 2 , V 2 ) d α 1 d α 2 N 1 1965 / 1008 + ϵ ( α 1 , α 2 ) [ 0 , 1 ] 2 | G ( α 1 + α 2 ) | λ L f ( α 2 , N 2 ) g ( α 2 , N 2 ) S ( α 2 , U 2 ) T ( α 2 , V 2 ) d α 1 d α 2 ,

where we use the bound from [10, Lemma 2.5] and [13, Lemma 2.5] as follows:

sup α 1 C ( M 1 ) f ( α 1 , N 1 ) N 1 17/18 + ϵ , sup α 1 C ( M 1 ) g ( α 1 , N 1 ) N 1 7/16 + ϵ , sup α 1 C ( M 1 ) S ( α 1 , U 1 ) N 1 13/42 + ϵ , sup α 1 C ( M 1 ) T ( α 1 , V 1 ) N 1 65/252 + ϵ .

By using the integral transformation of β = α 1 + α 2 and the periodicity of G ( β ) , we have

( α 1 , α 2 ) [ 0 , 1 ] 2 G ( α 1 + α 2 ) λ L f ( α 2 , N 2 ) g ( α 2 , N 2 ) S ( α 2 , U 2 ) T ( α 2 , V 2 ) d α 1 d α 2 = 0 1 f ( α 2 , N 2 ) g ( α 2 , N 2 ) S ( α 2 , U 2 ) T ( α 2 , V 2 ) β [ α 2 , 1 + α 2 ] | G ( β ) | λ L d β d α 2 .

By the simple orthogonality and [14, Lemma 4.12], we have

0 1 f 2 ( α 2 , N 2 ) d α 2 N 2 1 + ϵ

and

0 1 g 2 ( α 2 , N 2 ) S 2 ( α 2 , U 2 ) T 2 ( α 2 , V 2 ) d α 2 N 2 11 / 9 + ϵ .

From Lemma 2.4 and Cauchy’s inequality, we have

( α 1 , α 2 ) [ 0 , 1 ] 2 G ( α 1 + α 2 ) | λ L f ( α 2 , N 2 ) g ( α 2 , N 2 ) S ( α 2 , U 2 ) T ( α 2 , V 2 ) d α 1 d α 2 N 2 10 / 9 + ϵ N 1 E ( λ ) .

We choose λ = 0.9322 and get

1 N 1 1965 / 1008 845 / 1008 ϵ N 2 N 1 10 / 9 ϵ N 2 10 / 9 ,

since N 2 N 1 > N 2 . Similarly,

2 N 2 1965 / 1008 845 / 1008 ϵ N 1 N 2 10 / 9 ϵ N 1 10 / 9 .

Then,

R 2 ( N 1 , N 2 ) N 1 10 / 9 ϵ N 2 10 / 9 L k + N 1 10 / 9 N 2 10 / 9 ϵ L k N 1 10 / 9 N 2 10 / 9 L k 1 .

Lemma 2.6

For every pair of sufficiently large even integers N 1 and N 2 satisfying N 2 N 1 > N 2 ,

R 3 ( N 1 , N 2 ) 260.757 λ k 9 N 1 10 / 9 N 2 10 / 9 L k .

Proof

First, we need to estimate

I = ( α 1 , α 2 ) [ 0 , 1 ] 2 g 4 ( α 1 , N 1 ) g 4 ( α 2 , N 2 ) G 28 ( α 1 + α 2 ) d α 1 d α 2 .

Following the lines in [14], we note that

I = h Z r 14 ( h ) M 1 p 1 2 , p 2 2 , p 3 2 , p 4 2 N 1 M 2 p 5 2 , p 6 2 , p 7 2 , p 8 2 N 2 p 2 2 + p 3 2 p 3 2 p 4 2 = h p 5 2 + p 6 2 p 7 2 p 8 2 = h i = 1 8 log p i ,

where

r 14 ( h ) = 4 ν j , μ j L j = 1 14 2 ν j 2 μ j = h 1 .

Let

S ( h ) = p > 2 1 + B ( p , h ) ( p 1 ) 4 ,

where

B ( p , h ) = a = 1 ( a , q ) = 1 q C 2 ( p , a ) 4 e ( a h / p ) .

As in the proof of [14, Lemma 3.2], we treat the case h 0 and h = 0 separately and obtain

I 128 2 N 1 N 2 h 0 r 14 ( h ) S 2 ( h ) + O ( N 1 N 2 L 26 ) .

Next, we estimate h 0 r 14 ( h ) S 2 ( h ) . Note that

B ( p , h ) = ( p + 1 ) 2 , if p 3 mod 4 and p h , ( p 2 + 6 p + 1 ) 4 p ( p + 1 ) h p , if p 1 mod 4 and p h , ( p 1 ) ( p + 1 ) 2 , if p 3 mod 4 and p | h , ( p 1 ) ( p 2 + 6 p + 1 ) , if p 1 mod 4 and p | h .

Then, from the proof of [14, Lemma 4.3] we have

S 2 ( h ) 8.54 κ 2 ( h ) p > 5 p | h 1 + b ( p ) ( p 1 ) 4 1 + a ( p ) ( p 1 ) 4 2 ,

where

κ ( h ) = 25 + 15 h 5 32 , if 3 | h , 5 h , 3 2 , if 15 | h , 0 , if 3 h , a ( p ) = ( p + 1 ) 2 , if p 3 mod 4 , 3 p 2 2 p 1 , if p 1 mod 4 , b ( p ) = ( p 1 ) ( p + 1 ) 2 , if p 3 mod 4 , ( p 1 ) ( p 2 + 6 p + 1 ) , if p 1 mod 4 .

Define the multiplicative function c ( d ) by

1 + 1 c ( p ) = 1 + b ( p ) ( p 1 ) 4 1 + a ( p ) ( p 1 ) 4 2 ,

where d is square-free and ( 30 , d ) = 1 . Then,

h 0 r 14 ( h ) S 2 ( h ) 8.54 ( h ) h 0 mod 3 κ 2 ( h ) p > 5 p | h 1 + 1 c ( p ) 8.54 ( h ) h 0 mod 3 5 h 25 + 15 h 5 32 2 p > 5 p | h 1 + 1 c ( p ) + 8.54 ( h ) h 0 mod 15 3 2 2 p > 5 p | h 1 + 1 c ( p ) = 8.54 ( h ) h 0 mod 3 25 2 + 15 2 32 2 p > 5 p | h 1 + 1 c ( p ) + 8.54 ( h ) h 0 mod 15 3 2 2 25 32 2 p > 5 p | h 1 + 1 c ( p ) = 7.09 ( h ) h 0 mod 3 p > 5 p | h 1 + 1 c ( p ) + 14 ( h ) h 0 mod 15 p > 5 p | h 1 + 1 c ( p ) 7.09 Σ 1 + 14 Σ 2 ,

where the condition ( h ) in ( h ) denotes that the summation is taken over all ν 1 , , ν 14 , μ 1 , , μ 14 satisfying 4 ν j , μ j L and h = j = 1 14 ( 2 ν j μ j ) 0 .

Let us consider Σ 1 . We have

Σ 1 d < N ϵ p | d p >5 μ 2 ( d ) c ( d ) 4 ν j , μ j L 1 j 14 3 d | h 1 + O ( N ϵ ) L 28 d < N ϵ p | d p >5 μ 2 ( d ) c ( d ) 1 ϱ (3 d ) 28 4 ν j , μ j ϱ (3 d ) 1 j 14 3 d | h 1 + O ( ϵ ) L 28 + O ( N ϵ ) ( c 1 + ϵ ) L 28 ,

where ϱ ( q ) denotes the smallest positive integer ϱ , such that 2 ϱ ( q ) 1 mod q and c 1 is a constant, which we will deal with later. Similarly, Σ 2 ( c 2 + ϵ ) L 28 , where c 2 is a constant. Set

β ( d ) = 1 ϱ ( 3 d ) 28 4 ν j , μ j ϱ ( 3 d ) 1 j 14 3 d | h 1 1

and m ( x ) = e x 2 e 1 . Then, we have

p | d p >5 β ( d ) x μ 2 ( d ) c ( d ) p >5 p | m ( x ) 1 + 1 c ( p ) p >5 1 + 1 c ( p ) 1 + 1 p 1 2 p >5 p | m ( x ) 1 + 1 p 1 2 8 15 2 c 3 e 2 γ log 2 x ,

where we use the fact m ( x ) / ϕ ( m ( x ) ) e γ log x for x 9 . Here, c 3 = p > 5 1 + 1 c ( p ) 1 + 1 p 1 2 1.3904 2 can be found in the proof of [14, Lemma 4.1]. With M = 35 , we have

c 1 = 2 M + M p | d p > 5 β ( d ) x μ 2 ( d ) c ( d ) d x x 2 p | d p > 5 β ( d ) M μ 2 ( d ) c ( d ) 1 β ( d ) 1 M + 8 15 2 c 3 e 2 γ ( 1 + log M ) 2 M 1.12031 .

The constant c 2 1.10302 can be handled in the similar way. Then, the numerical computations provide

h 0 r 14 ( h ) S 2 ( h ) 23.39 L 28 .

So we get

I 3.83 × 10 5 N 1 N 2 L 28 + O N 1 N 2 L 26 .

Next, by [11, Lemma 2.3] and [9, Lemma 2.5] we have

( α 1 , α 2 ) [ 0 , 1 ] 2 f 2 ( α 1 , N 1 ) f 2 ( α 2 , N 2 ) G 4 ( α 1 + α 2 ) d α 1 d α 2 305.8869 N 1 N 2 L 4

and

( α 1 , α 2 ) [0,1] 2 S 4 ( α 1 , U 1 ) T 4 ( α 1 , V 1 ) S 4 ( α 2 , U 2 ) T 4 ( α 2 , V 2 ) d α 1 d α 2 0 1 S ( α 1 , U 1 ) T ( α 1 , V 1 ) 4 d α 1 0 1 S ( α 2 , U 2 ) T ( α 2 , V 2 ) 4 d α 2 0.1289 N 1 13/9 N 2 13/9

Thus,

R 3 ( N 1 , N 2 ) ( λ L ) k 9 ( α 1 , α 2 ) [ 0 , 1 ] 2 f ( α 1 , N 1 ) g ( α 1 , N 1 ) S ( α 1 , U 1 ) T ( α 1 , V 1 ) f ( α 2 , N 2 ) g ( α 2 , N 2 ) × S ( α 2 , U 2 ) T ( α 2 , V 2 ) G 9 ( α 1 + α 2 ) d α 1 d α 2 ( λ L ) k 9 ( α 1 , α 2 ) [ 0 , 1 ] 2 f 2 ( α 1 , N 1 ) f 2 ( α 2 , N 2 ) G 4 ( α 1 + α 2 ) d α 1 d α 2 1 2 × ( α 1 α 2 ) [ 0 , 1 ] 2 g 4 ( α 1 , N 1 ) g 4 ( α 2 , N 2 ) G 28 ( α 1 + α 2 ) d α 1 d α 2 1 4 × ( α 1 , α 2 ) [ 0 , 1 ] 2 S 4 ( α 1 , U 1 ) T 4 ( α 1 , V 1 ) S 4 ( α 2 , U 2 ) T 4 ( α 2 , V 2 ) d α 1 d α 2 1 4 260.757 λ k 9 N 1 10 / 9 N 2 10 / 9 L k .

Combining Lemmas 2.3, 2.5, and 2.6, we obtain

R ( N 1 , N 2 ) > 0.00101 N 1 10 / 9 N 2 10 / 9 L k 260.757 λ k 9 N 1 10 / 9 N 2 10 / 9 L k .

We therefore solve the inequality

R ( N 1 , N 2 ) > 0

and get k 187 . Consequently, we deduce that every pair of large even integers N 1 , N 2 satisfying N 2 N 1 > N 2 can be written in the form of (1.5) for k 187 . Thus, Theorem 1.1 follows.

Acknowledgments

This work was supported by the Natural Science Foundation of China (Grant No. 11761048), the Natural Science Foundation of Jiangxi Province of China (Grant No. 20192BAB201002), the key Project of Education Science Planning in Jiangxi Province of 2020 Annual (Grant No. 20ZD062), the Social Science Planning Project of Jiangxi Province of 2019 Annual (Grant No. 19JY29) and the Key Laboratory of Jiangxi Province for Numerical Simulation and Emulation Techniques Open Subject (Grant No. 19ZB01). The authors would like to express their thanks to the referee for many useful suggestions and comments on the manuscript.

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Received: 2019-10-02
Revised: 2020-03-20
Accepted: 2020-04-28
Published Online: 2020-07-06

© 2020 Yong Cai and Liqun Hu, published by De Gruyter

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

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  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
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