Home Power moments of automorphic L-functions related to Maass forms for SL3(ℤ)
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Power moments of automorphic L-functions related to Maass forms for SL3(ℤ)

  • Jing Huang , Huafeng Liu EMAIL logo and Deyu Zhang
Published/Copyright: August 31, 2021

Abstract

Let f be a self-dual Hecke-Maass eigenform for the group S L 3 ( Z ) . For 1 2 < σ < 1 fixed we define m ( σ ) ( 2 ) as the supremum of all numbers m such that

1 T L ( s , f ) m d t f , ε T 1 + ε ,

where L ( s , f ) is the Godement-Jacquet L-function related to f . In this paper, we first show the lower bound of m ( σ ) for 2 3 < σ < 1 . Then we establish asymptotic formulas for the second, fourth and sixth powers of L ( s , f ) as applications.

MSC 2010: 11F03; 11F66

1 Introduction

Let f be a self-dual Hecke-Maass eigenform for the group S L 3 ( Z ) of type ν = ( α , β ) . Then the Langlands’ parameters for f are

μ f ( 1 ) = α + 2 β 1 , μ f ( 2 ) = α β , μ f ( 3 ) = 1 2 α β .

It is known that f has the following Fourier-Whittaker expansion:

f ( z ) = γ U 2 ( Z ) S L 2 ( Z ) m 1 n 0 A f ( m , n ) m n W J M γ 0 0 1 z , ν , ψ 1 , 1 ,

where U 2 = 1 0 1 , W J ( z , ν , ψ 1 , 1 ) is the Jacquet-Whittaker function, ψ 1 , 1 is a character of U 3 ( R ) , M = diag ( m n , m , 1 ) and A f ( m , n ) are the Fourier coefficients of f . The function W J ( z , ν , ψ 1 , 1 ) represents an exponential decay in y 1 and y 2 for

z = 1 x 12 x 13 1 x 23 1 y 1 y 2 y 1 1 .

From Kim and Sarnak [1] and Sarnak [2] we know that

A f ( m , n ) m n 5 14 + ε .

From [3], the Rankin-Selberg theory shows that

m n 2 N A f ( m , n ) 2 f N .

Due to A f ( m , n ) = A f ˜ ( n , m ) , then

(1.1) m 2 n N A f ( m , n ) 2 f N

also holds, where f ˜ is the contragredient form of f . According to these estimates, we have

(1.2) m N A f ( m , 1 ) 2 m log N , n N A f ( 1 , n ) 2 n log N .

As in [4] and [5], the Godement-Jacquet L-function associated with f is defined as

L ( s , f ) = n = 1 A f ( 1 , n ) n s , for s > 1 .

This L-function has a standard functional equation and analytic continuation to an entire function on complex plane C . Due to the fact that f is a Hecke eigenform, the Fourier coefficients are multiplicative and the L-function has an Euler product (see [5, pp. 173–174]), for s > 1 ,

L ( s , f ) = p ( 1 A f ( 1 , p ) p s + A f ( p , 1 ) p 2 s p 3 s ) 1 .

Then the L-function associated with the dual Maass form f ˜ takes the form

L ( s , f ˜ ) = n = 1 A f ( n , 1 ) n s = p ( 1 A f ( p , 1 ) p s + A f ( 1 , p ) p 2 s p 3 s ) 1 .

We write s = σ + i t and suppose that 1 2 < σ < 1 is fixed. Let m ( σ ) ( 2 ) be the supremum of all numbers m ( 2 ) such that

(1.3) 1 T L ( s , f ) m d t f , ε T 1 + ε ,

where the -constant may depend on L ( s , f ) and ε . Naturally, we want to seek lower bounds for m ( σ ) , which occurs frequently in applications. In the cases of full modular group S L 2 ( Z ) and the congruence group, many scholars have obtained lot of results (e.g., see [6,7,8, 9,10,11, 12,13,14, 15,16,17, 18,19,20, 21,22,23, 24,25], etc.).

In this paper, we focus our attention on the Hecke-Maass eigenforms for the group S L 3 ( Z ) . In this situation, for one thing, we do not know whether the Ramanujan conjecture is true; for another, the square and fourth mean value estimates of L ( s , f ) are weaker than ones over S L 2 ( Z ) . Our results are as follows.

Theorem 1

Let m ( σ ) for each 2 3 < σ < 1 be defined by (1.3). Then we have

(1.4) m ( σ ) 4 ( 3 2 σ ) 5 ( 4 3 σ ) ( 1 σ ) .

From Theorem 1 we can get the following corollary immediately.

Corollary

We have

m 2 3 2 , m 97 769 90 3 , , m 103 349 90 12 , .

Remark

Due to the fact that L ( s , f ) is an L-function of degree 3, then Perelli’s mean value theorem [26] shows that, for 1 2 σ 1 and T 1 uniformly,

1 T L ( σ + i t , f ) 2 d t T max ( 3 ( 1 σ ) , 1 ) + ε ,

which implies

1 T L ( σ + i t , f ) 2 d t T 1 + ε 2 3 σ 1 .

Thus, we restrict the range of σ in Theorem 1 into 2 3 < σ < 1 .

As applications of Theorem 1, we can establish the asymptotic formulas for the second, fourth and sixth powers of L ( s , f ) .

Theorem 2

For any ε > 0 and σ fixed, we have

(1.5) 1 T L ( σ + i t , f ) 2 d t = T n = 1 A f ( 1 , n ) 2 n 2 σ + O T 4 3 σ 2 + ε ,

(1.6) 1 T L ( σ + i t , f ) 4 d t = T n = 1 A f A f ( 1 , n ) 2 n 2 σ + O T 27 + 69 30 σ 2 69 6 + ε ,

(1.7) 1 T L ( σ + i t , f ) 6 d t = T n = 1 A f A f A f ( 1 , n ) 2 n 2 σ + O T 79 + 481 90 σ 2 481 22 + ε ,

where A f A f ( 1 , n ) = n = m l A f ( 1 , m ) A f ( 1 , l ) is the Dirichlet convolution of A f ( 1 , n ) with itself. The asymptotic formulas (1.5), (1.6) and (1.7) follow for 2 3 < σ < 1 , 33 69 30 < σ < 1 and 101 481 90 < σ < 1 , respectively.

Notation. Throughout this paper, the letter ε stands for a sufficiently small positive number, and the value of ε may change from statement to statement.

2 Some lemmas

In order to prove Theorems 1 and 2, we first introduce some lemmas.

Lemma 2.1

Let T t 2 T and k 1 be a fixed integer. Then for 1 2 < σ < 1 , we have

L ( σ + i t , f ) k 1 + log T log 2 T log 2 T L ( σ 1 log T + i t + i v , f ) k e v d v .

Proof

The proof of this lemma is similar to [27, Lemma 7.1], and we just need to use the following functional equation:

G ν ( s ) L ( s , f ) = G ˜ ν ( 1 s ) L ( 1 s , f ˜ ) ,

where

G ν ( s ) = π 3 s 2 Γ s + 1 2 α β 2 Γ s + α β 2 Γ s 1 + α + 2 β 2 , G ˜ ν ( s ) = π 3 s 2 Γ s + 1 α 2 β 2 Γ s α + β 2 Γ s 1 + 2 α + β 2 ,

in place of the functional equation of ζ ( s ) .□

Lemma 2.2

For m = m ( σ ) ,

(2.1) 1 T L ( σ + i t , f ) m ( σ ) d t T 1 + ε

is equivalent to

(2.2) r R L ( σ + i t r , f ) m ( σ ) T 1 + ε ,

where

(2.3) t r [ T , 2 T ] for r = 1 , , R ; t r t s log 4 T for 1 r s R .

Proof

Let

L ( σ + i t m , f ) = max t I m L ( σ + i t , f ) , I m = [ 2 T m log 4 T , 2 T ( m 1 ) log 4 T ] ,

where m = 1 , 2 , , [ T log 4 T ] . Denote by { t r } either of the sets { t 2 m } or { t 2 m 1 } . Then the t r ’s satisfy (2.3) and

T 2 T L ( σ + i t , f ) m ( σ ) d t m = 1 [ t log 4 T ] 2 T m log 4 T 2 T ( m 1 ) log 4 T L ( σ + i t m , f ) m ( σ ) d t m = 1 [ t log 4 T ] L ( σ + i t m , f ) m ( σ ) log 4 T T 1 + ε .

And then replacing T by T 2 , T 2 2 , and adding we can get (2.1). On the other hand, by Lemma 2.1, we have

r R L ( σ + i t r , f ) m ( σ ) d t R + log T r R log 2 T log 2 T L ( σ 1 log T + i t r + i v , f ) m ( σ ) d v R + log T r R t r log 2 T t r + log 2 T L ( σ 1 log T + i t , f ) m ( σ ) d t T log 4 T + log T 1 2 T + log 2 T L ( σ 1 log T + i t , f ) m ( σ ) d t T 1 + ε ,

which implies (2.1).□

Lemma 2.3

We suppose that 1 2 < σ < 1 is fixed and

(2.4) R T 1 + ε V m ( σ ) ,

where for t r defined by (2.3) we have

(2.5) L ( σ + i t r , f ) V T ε ( r = 1 , 2 , , R ) ,

which is equivalent to

(2.6) r R L ( σ + i t r , f ) m ( σ ) T 1 + ε .

Proof

We suppose that (2.6) is true and let { t V , 1 , , t V , R 1 } be the subset of { t r } such that

L ( σ + i t V , j , f ) V ( j = 1 , , R 1 ) .

Then from (2.6) we have

R 1 V m ( σ ) r R L ( σ + i t r , f ) m ( σ ) T 1 + ε ,

thus for R 1 = R , (2.4) holds.

Inversely, we let (2.4) hold and denote by t V , 1 , , t V , R ( V ) those of the points t 1 , , t R for which

V L ( σ + i t V , j , f ) 2 V ( j = 1 , , R ( V ) ) .

For each V , we have O ( log T ) choices. And from the following Lemma 2.6, we take V = T 5 ( 1 σ ) 4 , V = 2 1 T 5 ( 1 σ ) 4 , V = 2 2 T 5 ( 1 σ ) 4 , . Then we can obtain

r R L ( σ + i t r , f ) m ( σ ) d t R T ε + V j R ( V ) ( 2 V ) m ( σ ) R T ε + V T 1 + ε T 1 + ε .

Lemma 2.4

Let t 1 < < t R be real numbers such that t r [ T , 2 T ] for r = 1 , , R ; t r t s log 4 T for 1 r s R . If

(2.7) T ε V M < n 2 M a ( n ) n σ i t r ,

where n M a ( n ) 2 M 1 + ε for 1 M T C ( C > 0 ) , then we have

(2.8) R T ε ( M 2 2 σ V 2 + T V f ( σ ) ) ,

where

(2.9) f ( σ ) = 2 3 4 σ , if 1 2 < σ 2 3 , 10 7 8 σ , if 2 3 σ 11 14 , 34 15 16 σ , if 11 14 σ 13 15 , 98 31 32 σ , if 13 15 σ 57 62 , 5 1 σ , if 57 62 σ 1 ε .

Proof

We can get this lemma by following a similar argument to [6, Lemma 8.2] replacing a ( n ) M ε by n M a ( n ) 2 M 1 + ε .□

Lemma 2.5

[27, Theorem 5.2] Let a 1 , , a N be arbitrary complex numbers. Then

0 T n N a n n i t 2 d t = T n N a n 2 + O n N n a n 2 ,

and the above formula remains also valid if N = , provided that the series on the right hand side of the aforementioned formula converge.

Lemma 2.6

[28, Corollary 1.2] Let 1 2 σ 1 be fixed, we have

L ( σ + i t , f ) t 5 4 ( 1 σ ) + ε .

Lemma 2.7

For any ε > 0 , we have

0 T L 2 3 + i t , f 2 d t T 1 + ε , 0 T L 2 3 + i t , f 4 d t T 17 12 + ε .

Proof

The first result is a general result of Perelli [26], which we can also get from Lemma 2.5 with m = 3 and σ = 2 3 in Liu and Zhang [29]. From Lemma 2.6 and the first result, we can easily get the second result.□

Lemma 2.8

For t r satisfying (2.3), we have

r R L 2 3 + i t r , f 2 d t T 1 + ε , r R L 2 3 + i t r , f 4 d t T 17 12 + ε .

Proof

Following a similar argument of Lemma 2.2, with the help of Lemma 2.7 we can obtain this lemma.□

Lemma 2.9

[27, Lemma 8.3] Let F ( s ) be regular in the region D : α σ β , t 1 and let F ( s ) e C t 2 for s D . Then for any fixed q > 0 and α < γ < β , we have

2 T F ( γ + i t ) q d t 1 2 T F ( α + i t ) q d t + 1 β γ β α 1 2 T F ( β + i t ) q d t + 1 γ α β α .

In the following two lemmas, though the definitions of φ k ( m ) and ψ k ( n ) are different from ones in Lemmas 2.11 and 2.12 of [18], we still can get these two lemmas by following similar arguments, respectively.

Lemma 2.10

Let φ k ( n ) be the arithmetic function generated by L ( s , f ) k , that is

(2.10) φ k ( n ) = A f A f ( 1 , n ) k times .

Then we have

n x φ k ( n ) x 1 + ε , n x φ k 2 ( n ) x 1 + ε .

Lemma 2.11

Let 0 < δ < 1 2 be a fixed constant and

ψ k ( n ) = φ 2 k ( n ) n = m l m T , l T φ k ( m ) φ k ( l ) , T < n T 2 , φ 2 k ( n ) , n > T 2 .

Then we have

n T ψ k 2 ( n ) n 2 2 δ = O ( 1 ) .

3 Proofs of Theorems 1 and 2

3.1 Proof of Theorem 1

In this section, we restrict the range of σ into 2 3 < σ < 1 and shall give lower bounds for m ( σ ) by establishing formulas of type

R T 1 + ε V m ( σ ) .

Recalling Mellin’s formula

(3.1) e x = ( 2 π i ) 1 2 i 2 + i Γ ( ω ) x ω d ω ( x > 0 ) .

Taking x = n Y and multiplying (3.1) by A f ( 1 , n 1 ) A f ( 1 , n 2 ) n 1 s n 2 s , where n = n 1 n 2 and summing over n , we can obtain

(3.2) n = 1 n = n 1 n 2 A f ( 1 , n 1 ) A f ( 1 , n 2 ) e n Y n s = ( 2 π i ) 1 2 i 2 + i Y ω Γ ( ω ) L ( s + ω , f ) 2 d ω .

Shifting the line of integration in (3.2) to ω = 2 3 σ , we encounter a simple pole at ω = 0 with residue L ( s , f ) 2 and get, as Y ,

(3.3) n Y log 2 Y n = n 1 n 2 A f ( 1 , n 1 ) A f ( 1 , n 2 ) e n Y n s + o ( 1 ) = L ( s , f ) 2 + ( 2 π i ) 1 ω = 2 3 σ Y ω Γ ( ω ) L ( s + ω , f ) 2 d ω .

The integral part of (3.3) for which ω log 2 T is o ( 1 ) as T by Stirling’s formula. Then let s = σ + i t r and thus for each t r we have

(3.4) L ( σ + i t r , f ) 2 1 + n Y log 2 Y n = n 1 n 2 A f ( 1 , n 1 ) A f ( 1 , n 2 ) e n Y n σ i t r + log 2 T log 2 T Y 2 3 σ L 2 3 + i t r + i v , f 2 e v d v .

Combining (2.5) with (3.4), we can obtain

(3.5) V 2 n Y log 2 Y n = n 1 n 2 A f ( 1 , n 1 ) A f ( 1 , n 2 ) e n Y n σ i t r log T max M 1 2 Y log 2 Y M < n 2 M n = n 1 n 2 A f ( 1 , n 1 ) A f ( 1 , n 2 ) e n Y n σ i t r

or

(3.6) V 2 Y 2 3 σ L 2 3 + i t r , f 2 ,

where V T ε and t r is defined as

L 2 3 + i t r , f = max log 2 T v log 2 T L 2 3 + i t r + i v , f .

For convenience, denote by R 1 and R 2 those points which satisfy (3.5) and (3.6), respectively.

Recalling (1.1), we know that Lemma 2.4 is valid. We first consider R 1 . By Lemma 2.4, we have

(3.7) R 1 log Y × T ε ( M 2 2 σ V 4 + T V 2 f ( σ ) ) T ε ( Y 2 2 σ V 4 + T V 2 f ( σ ) ) .

While for R 2 , by Lemma 2.8, Hölder’s inequality and (3.6), we can obtain

(3.8) R 2 Y 2 3 σ V 2 r R 2 L 2 3 + i t r , f 2 Y 2 3 σ V 2 T 1 + ε

and

(3.9) R 2 Y 2 3 σ V 2 r R 2 L 2 3 + i t r , f 2 Y 2 3 σ V 2 R 2 1 2 T 17 24 + ε .

For (3.8), if we take Y = V 6 4 3 σ T 3 4 3 σ , then we have

(3.10) R R 1 + R 2 T ε Y 2 2 σ V 4 + T V 2 f ( σ ) + Y 2 3 σ V 2 T 1 + ε T ε V 4 4 3 σ T 6 6 σ 4 3 σ + T V 2 f ( σ ) .

For (3.9), if we take Y = T 17 8 , then we have

(3.11) R R 1 + R 2 T ε Y 2 2 σ V 4 + T V 2 f ( σ ) + Y 4 3 2 σ V 4 T 17 12 T ε V 4 T 17 4 17 4 σ + T V 2 f ( σ ) .

Therefore, combining (3.10) with (3.11) we have

(3.12) R T ε T V 2 f ( σ ) + V 4 4 3 σ T 6 6 σ 4 3 σ + V 4 T 17 4 17 4 σ .

We assume that the second and the third terms in (3.12) do not exceed T V x and T V y , for values x and y which can be determined by Lemma 2.6, then we can obtain

x 4 ( 3 2 σ ) 5 ( 1 σ ) ( 4 3 σ ) , y 7 3 σ 5 ( 1 σ ) .

Thus, we have

R T 1 + ε V z

with

z = min 2 f ( σ ) , 4 ( 3 2 σ ) 5 ( 1 σ ) ( 4 3 σ ) , 7 3 σ 5 ( 1 σ ) .

For 2 3 < σ 1 ε , we always have

4 ( 3 2 σ ) 5 ( 1 σ ) ( 4 3 σ ) < 7 3 σ 5 ( 1 σ ) .

Recalling the value of f ( σ ) in Lemma 2.4, we can take

z = 4 ( 3 2 σ ) 5 ( 1 σ ) ( 4 3 σ ) , 2 3 < σ 1 ε .

Thus, we complete the proof of Theorem 1.

3.2 Proof of Theorem 2

In this section, we give the proof of Theorem 2 by following a similar argument to [6, Theorem 2]. Let σ k denote the infimum of all numbers σ for which

1 T L ( σ + i t , f ) 2 k d t T 1 + ε

holds for any ε > 0 , where k 1 is a fixed integer, 1 2 σ k < 1 .

Writing s = σ + i t , we have

(3.13) 1 T L ( σ + i t , f ) 2 k d t = 1 T n T φ k ( n ) n σ i t 2 d t + O 1 T L ( σ + i t , f ) n T φ k ( n ) n σ i t 2 d t ,

where φ k ( n ) is given by Lemma 2.10.

Combining Abel’s summation formula with Lemmas 2.5 and 2.10, we can obtain

(3.14) 1 T n T φ k ( n ) n σ i t 2 d t = T n T φ k 2 ( n ) n 2 σ + O n T φ k 2 ( n ) n 1 2 σ = T n = 1 φ k 2 ( n ) n 2 σ + O ( T 2 2 σ + ε ) .

Let

F ( σ + i t , f ) = L 2 k ( σ + i t , f ) n T φ k ( n ) n σ i t 2 .

And applying Lemma 2.9 with q = 1 , α = σ k + δ , β = 1 + δ , γ = σ , where 0 < δ < 1 2 is a fixed constant which may be chosen arbitrarily small, for fixed k we have

β σ β α = 1 + δ σ 1 σ k 1 σ 1 σ k + δ 1 2

and

σ α β α = σ σ k δ 1 σ k σ σ k 1 σ k .

Recalling the definition of σ k , by Lemma 2.5 we have

1 2 T F ( α + i t , f ) d t 1 2 T L ( σ k + δ + i t , f ) 2 k d t + 1 2 T n T φ k ( n ) n σ k δ i t 2 d t T 1 + δ + T 2 2 σ k + ε T 1 + δ .

Moreover,

F ( β + i t , f ) = n = 1 φ 2 k ( n ) n 1 δ i t n T φ k ( n ) n 1 δ i t 2 = n > T ψ k ( n ) n 1 δ i t ,

where ψ k ( n ) is given by Lemma 2.11.

By Lemma 2.5, Lemma 2.10 and Hölder’s inequality, we can obtain

1 2 T F ( β + i t , f ) d t T 1 2 1 2 T n T ψ k ( n ) n 1 δ i t 2 d t 1 2 T 1 2 .

Thus, Lemma 2.9 shows

1 2 T F ( σ + i t , f ) d t T ( 1 + δ ) 1 σ 1 σ k + δ 1 2 + σ σ k 2 2 σ k .

Note that

( 1 + δ ) 1 σ 1 σ k + δ 1 2 + σ σ k 2 2 σ k 2 σ σ k 2 2 σ k + ε

holds for any ε > 0 if δ = δ ( ε ) is sufficiently small. Noting that for the exponent of the O -term in (3.14), we have

2 2 σ < 2 σ σ k 2 2 σ k < 1 .

Thus,

1 T L ( σ + i t , f ) 2 k d t = T n = 1 φ k 2 ( n ) n 2 σ + R ( k , σ ; T ) ,

and for fixed σ satisfying σ k < σ < 1 , we have

R ( k , σ ; T ) T 2 σ σ k 2 2 σ k + ε .

From Theorem 1 we have

1 T L 2 3 + i t , f 2 d t T 1 + ε , 1 T L 33 69 30 + i t , f 4 d t T 1 + ε , 1 T L 101 481 90 + i t , f 6 d t T 1 + ε .

Recalling the definition of σ k , we can take σ 1 = 2 3 , σ 2 = 33 69 30 and σ 3 = 101 481 90 , from which we can obtain Theorem 2 immediately.

Acknowledgment

The authors are greatly indebted to the reviewers for very beneficial suggestions and comments which led to essential improvement of the original version of this paper. This work was supported by the National Natural Science Foundation of China (Grant Nos. 11771256 and 11801328).

  1. Conflict of interest: Authors state no conflict of interest.

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Received: 2020-09-30
Revised: 2021-06-16
Accepted: 2021-07-12
Published Online: 2021-08-31

© 2021 Jing Huang et al., published by De Gruyter

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

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  2. Sharp conditions for the convergence of greedy expansions with prescribed coefficients
  3. Range-kernel weak orthogonality of some elementary operators
  4. Stability analysis for Selkov-Schnakenberg reaction-diffusion system
  5. On non-normal cyclic subgroups of prime order or order 4 of finite groups
  6. Some results on semigroups of transformations with restricted range
  7. Quasi-ideal Ehresmann transversals: The spined product structure
  8. On the regulator problem for linear systems over rings and algebras
  9. Solvability of the abstract evolution equations in Ls-spaces with critical temporal weights
  10. Resolving resolution dimensions in triangulated categories
  11. Entire functions that share two pairs of small functions
  12. On stochastic inverse problem of construction of stable program motion
  13. Pentagonal quasigroups, their translatability and parastrophes
  14. Counting certain quadratic partitions of zero modulo a prime number
  15. Global attractors for a class of semilinear degenerate parabolic equations
  16. A new implicit symmetric method of sixth algebraic order with vanished phase-lag and its first derivative for solving Schrödinger's equation
  17. On sub-class sizes of mutually permutable products
  18. Asymptotic solution of the Cauchy problem for the singularly perturbed partial integro-differential equation with rapidly oscillating coefficients and with rapidly oscillating heterogeneity
  19. Existence and asymptotical behavior of solutions for a quasilinear Choquard equation with singularity
  20. On kernels by rainbow paths in arc-coloured digraphs
  21. Fully degenerate Bell polynomials associated with degenerate Poisson random variables
  22. Multiple solutions and ground state solutions for a class of generalized Kadomtsev-Petviashvili equation
  23. A note on maximal operators related to Laplace-Bessel differential operators on variable exponent Lebesgue spaces
  24. Weak and strong estimates for linear and multilinear fractional Hausdorff operators on the Heisenberg group
  25. Partial sums and inclusion relations for analytic functions involving (p, q)-differential operator
  26. Hodge-Deligne polynomials of character varieties of free abelian groups
  27. Diophantine approximation with one prime, two squares of primes and one kth power of a prime
  28. The equivalent parameter conditions for constructing multiple integral half-discrete Hilbert-type inequalities with a class of nonhomogeneous kernels and their applications
  29. Boundedness of vector-valued sublinear operators on weighted Herz-Morrey spaces with variable exponents
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  31. Quantum Ostrowski-type inequalities for twice quantum differentiable functions in quantum calculus
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  33. Infinitesimals via Cauchy sequences: Refining the classical equivalence
  34. The (1, 2)-step competition graph of a hypertournament
  35. Properties of multiplication operators on the space of functions of bounded φ-variation
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  50. Inhomogeneous conformable abstract Cauchy problem
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  53. Symmetric graphs of valency seven and their basic normal quotient graphs
  54. Mean oscillation and boundedness of multilinear operator related to multiplier operator
  55. Numerical methods for time-fractional convection-diffusion problems with high-order accuracy
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  57. Finite groups whose intersection power graphs are toroidal and projective-planar
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  59. A note on polyexponential and unipoly Bernoulli polynomials of the second kind
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  61. Some estimates for commutators of Littlewood-Paley g-functions
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  143. Special Issue on Fractional Problems with Variable-Order or Variable Exponents (Part I)
  144. On the mixed fractional quantum and Hadamard derivatives for impulsive boundary value problems
  145. The Lp dual Minkowski problem about 0 < p < 1 and q > 0
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