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Constructions of pseudorandom binary lattices using cyclotomic classes in finite fields

  • Xiaolin Chen EMAIL logo
Published/Copyright: December 29, 2020

Abstract

In 2006, Hubert, Mauduit and Sárközy extended the notion of binary sequences to n-dimensional binary lattices and introduced the measures of pseudorandomness of binary lattices. In 2011, Gyarmati, Mauduit and Sárközy extended the notions of family complexity, collision and avalanche effect from binary sequences to binary lattices. In this paper, we construct pseudorandom binary lattices by using cyclotomic classes in finite fields and study the pseudorandom measure of order k, family complexity, collision and avalanche effect. Results indicate that such binary lattices are “good,” and their families possess a nice structure in terms of family complexity, collision and avalanche effect.

MSC 2010: 11K45; 11B50; 94A55; 94A60

1 Introduction

The need for pseudorandom binary lattices arises in many applications, so numerous papers have been written on this subject. In these papers, some measures are introduced and studied. For example, Hubert, Mauduit and Sárközy [1] extended the notion of binary sequences to n-dimensional binary lattices and introduced the measures of pseudorandomness of binary lattices. For details, let I N n denote the set of n-dimensional vectors all whose coordinates are in { 0 , 1 , , N 1 } . That is,

I N n = { x = ( x 1 , , x n ) : x 1 , , x n { 0 , 1 , , N 1 } } .

A function of the type η ( x ) = η ( ( x 1 , , x n ) ) : I N n { 1 , + 1 } is called an n-dimensional binary N-lattice or briefly a binary lattice.

Let k , and u i ( i = 1 , , n ) denote the n-dimensional unit vector whose ith coordinate is 1 and the others are 0. Write

k ( η ) = max B , d 1 , , d k , T j 1 = 0 t 1 j n = 0 t n η j 1 b 1 u 1 + + j n b n u n + d 1 × × η j 1 b 1 u 1 + + j n b n u n + d k ,

where the maximum is taken over all n-dimensional vectors B = ( b 1 , , b n ) , d 1 , , d k , T = ( t 1 , , t n ) such that their coordinates are non-negative integers, b 1 , , b n are non-zero, d 1 , , d k are distinct and all the points j 1 b 1 u 1 + + j n b n u n + d i occurring in the multiple sum belong to I N n . Then k ( η ) is called the pseudorandom measure of order k of η .

An n-dimensional binary N-lattice η is considered as a “good” pseudorandom binary lattice if k ( η ) is “small” in terms of N for small k. This terminology is justified since Hubert, Mauduit and Sárközy [1] proved that for a fixed k and for a truly random n-dimensional binary N-lattice η we have

N n 2 k ( η ) N n 2 ( log N n ) 1 2

with probability greater than 1 ε , while the trivial upper bound for k ( η ) is N n .

In 2011, Gyarmati, Mauduit and Sárközy [2] extended the notions of family complexity, collision and avalanche effect from binary sequences to binary lattices.

Assume that n , N , and is a family of n-dimensional binary N-lattices η : I N n { 1 , + 1 } . Let j N n , x 1 , x 2 , , x j I N n be j distinct vectors, and ( ε 1 , ε 2 , , ε j ) { 1 , + 1 } j . The family complexity or f-complexity of the family , denoted by Γ ( ) , is defined as the greatest integer j such that for any specification of length j, there is at least one η satisfying

η ( x 1 ) = ε 1 , η ( x 2 ) = ε 2 , , η ( x j ) = ε j .

Obviously, we have the trivial bound

Γ ( ) log | | log 2 .

Assume that n , N , S is a given finite set (e.g., a set of certain polynomials), to each s S we assign a unique n-dimensional binary N-lattice η = η s : I N n { 1 , + 1 } , and let = ( S ) denote the family of the binary lattices obtained in this way:

(1.1) = ( S ) = η s : s S .

Definition 1.1

If s S , s S , s s , η s = η s , then this is said to be a collision in = ( S ) . If there is no collision in = ( S ) , then is said to be collision free.

Definition 1.2

If = ( S ) is of form (1.1), changing any element s S for any s S with s s changes “many” elements of η s : I N n { 1 , + 1 } , then we speak about the avalanche effect, and we say that = ( S ) possesses the avalanche property. If for any s S , s S , s s , there are at least 1 2 o ( 1 ) N n points x I N n such that η s ( x ) η s ( x ) , then is said to possess the strict avalanche property.

Definition 1.3

If n , N , η : I N n { 1 , + 1 } , η : I N n { 1 , + 1 } , then the distance d ( η , η ) between η and η is defined by

d ( η , η ) = | { x I N n : η ( x ) η ( x ) } | .

If = ( S ) is of form (1.1), then the distance minimum m ( ) in is defined by

m ( ) = min s , s S s s d ( η s , η s ) .

Clearly, is collision free if m ( ) > 0 , and possesses the strict avalanche property if

m ( ) 1 2 o ( 1 ) N n .

Many pseudorandom binary lattices have been obtained and studied by using the subsets in finite fields (see [1,2,3,4,5,6,7,8,9,10,11]). Suppose that q = p n is an odd prime power and F q is a finite field with q elements. Let v 1 , , v n be linearly independent elements of F q over F p and let α be a primitive element of the finite field F q , and d > 1 be a divisor of q 1 . The dth cyclotomic classes C i ( d , q ) of F q are defined by

C i ( d , q ) = { α j d + i : 0 j q 1 d 1 } ,

where 0 i d 1 . Then C 0 ( d , q ) is a subgroup of F q = F q \ { 0 } , and C i ( d , q ) = α i C 0 ( d , q ) , 0 i d 1 . The dth cyclotomic classes give a partition of F q

F q = i = 0 d 1 C i ( d , q ) .

In this paper, we shall give large families of binary lattices by using the cyclotomic classes in finite fields and study their properties. Our results are the following.

Theorem 1.1

Suppose that f ( x ) F q [ x ] with deg ( f ) < p has no multiple zero in F ¯ q , where F ¯ q is an algebraic closure of F q . Let d > 1 be a divisor of q 1 and d be even. Define

(1.2) η ( x 1 , , x n ) = + 1 , i f f ( x 1 v 1 + + x n v n ) { 0 } i = 0 d 2 1 C i ( d , q ) , 1 , i f f ( x 1 v 1 + + x n v n ) i = d 2 d 1 C i ( d , q ) ,

where x i { 0 , 1 , , N 1 } for any i { 1 , , n } . Assume that one of the following conditions holds

( a ) f i s i r r e d u c i b l e ; ( b ) k = 2 ; ( c ) 4 n ( d e g ( f ) + k ) < p .

Then we have

k ( η ) < k 2 2 k d e g ( f ) q 1 2 ( 1 + log p ) n log k ( 1 + d ) .

Theorem 1.2

Suppose that K , K < q , S denotes the set of all polynomials f ( x ) F q [ x ] with 0 < deg ( f ) K of which the multiplicity of each zero in F ¯ q is less than d. Let d > 1 be a divisor of q 1 and d be even. Define

(1.3) η f ( x 1 , , x n ) = + 1 , i f f ( x 1 v 1 + + x n v n ) { 0 } i = 0 d 2 1 C i ( d , q ) , 1 , i f f ( x 1 v 1 + + x n v n ) i = d 2 d 1 C i ( d , q ) ,

and = ( S ) = { η f : f S } . Then

Γ ( ) K .

Theorem 1.3

Suppose that S denotes the set of all monic polynomials f ( x ) F q [ x ] with 0 < deg ( f ) L which have no multiple zero in F ¯ q , and let d > 1 be a divisor of q 1 and d be even. Define

(1.4) η f ( x 1 , , x n ) = + 1 , i f f ( x 1 v 1 + + x n v n ) { 0 } i = 0 d 2 1 C i ( d , q ) , 1 , i f f ( x 1 v 1 + + x n v n ) i = d 2 d 1 C i ( d , q ) ,

and = ( S ) = { η f : f S } . Then

m ( ) q 2 8 ( 2 L 1 ) q 1 2 log 2 ( 1 + d ) L .

Corollary 1.1

Let , L be defined as in Theorem 1.3. If

L < q 2 + q 1 2 log 2 ( 1 + d ) 16 q 1 2 log 2 ( 1 + d ) + 1 ,

then is collision free. Furthermore, if

L = o q 1 2 ,

then possesses the strict avalanche property.

2 Estimates for character sums of polynomials

We need the following lemmas to prove the theorems.

Lemma 2.1

Suppose that F q is a finite field, α is a generator of the multiplicative group F q , and χ is a non-trivial multiplicative character such that χ d = χ 0 . Then

k = 0 d 1 χ ( α k ) = 0 .

Proof

This is Lemma 4A of [12].□

Lemma 2.2

Suppose that F q is a finite field and χ is a non-trivial multiplicative character of F q . Assume that f ( x ) F q [ x ] has m distinct ones among its zeros, and it is not a constant times of a ord ( χ ) th power. Then

z F q χ ( f ( z ) ) ( m 1 ) q 1 2 .

Proof

This is Theorem 2C′ of [12].□

Lemma 2.3

Suppose that q = p n is an odd prime power and F q is a finite field. Let z 1 , , z k F q and 0 δ 1 , , δ k < d but not every δ i be zero. Assume that f ( x ) F q [ x ] with deg ( f ) < p has no multiple zero in F ¯ q , and assume that one of the following conditions holds

( a ) f i s i r r e d u c i b l e ; ( b ) k = 2 ; ( c ) 4 n ( deg ( f ) + k ) < p .

Then

f δ 1 ( x + z 1 ) f δ k ( x + z k ) F q [ x ]

is not a constant times of a dth power of a polynomial.

Proof

This is Lemma 5 of [11].□

Lemma 2.4

Suppose that q = p n is a prime power and χ is a non-trivial multiplicative character of the finite field F q . Assume that a non-constant polynomial f ( x ) F q [ x ] has m distinct zeros in its splitting field over F q , and it is not a constant times of a ord ( χ ) th power. Let

B = j = 1 n j i v i : 0 j i t i , 0 t i p 1 , i = 1 , 2 , , n ,

where v 1 , , v n are linearly independent over F p . Then we get

z B χ ( f ( z ) ) < m q 1 2 ( 1 + log p ) n .

Proof

This is Theorem 2 of [13].□

Lemma 2.5

Suppose that q = p n is an odd prime power, α is a primitive element of the finite field F q and d > 1 be a divisor of q 1 . Let F q ^ denote the set of all multiplicative characters of F q and G = { χ F q ^ : χ d = χ 0 } \ { χ 0 } . For 0 y q 2 , the following bound holds

χ G j = x x + y χ ( α j ) < 2 d log ( 1 + d ) .

Proof

This is Lemma 1 of [14].□

Lemma 2.6

Suppose that T is a field and g ( x ) T [ x ] is a non-zero polynomial, then it can be written in the form

g ( x ) = ( h ( x ) ) k g ( x ) ,

where h ( x ) , g ( x ) T [ x ] and the multiplicity of each zero of g ( x ) in T ¯ is less than k.

Proof

This is Lemma 6 of [15].□

3 Pseudorandom measure of order k

Now we prove Theorem 1.1.

Let F q ^ denote the set of all multiplicative characters of F q and G = { χ F q ^ : χ d = χ 0 } . For ( x 1 , , x n ) with f ( ξ n ) = f ( x 1 v 1 + + x n v n ) 0 , by the orthogonality relations for characters and Lemma 2.1 we have

f ( ξ n ) i = 0 d 2 1 C i ( d , q ) there exist 0 i d 2 1 , 0 j q 1 d 1 satisfying f ( ξ n ) = α j d + i 1 q 1 i = 0 d 2 1 j = 0 q 1 d 1 χ F q ^ χ ¯ ( f ( ξ n ) ) χ ( α j d + i ) = 1 1 d i = 0 d 2 1 χ G χ ¯ ( f ( ξ n ) ) χ ( α i ) = 1 .

Write G = G \ { χ 0 } . Hence,

(3.1) η ( x 1 , , x n ) = 2 d χ G j = 0 d 2 1 χ ( α j ) χ ¯ ( f ( x 1 v 1 + + x n v n ) ) .

Define B = i = 1 n j i ( b i v i ) : 0 j i t i , 0 t i p 1 , i = 1 , 2 , , n , where b 1 , , b n are positive integers, and write d i = d 1 ( i ) , , d n ( i ) , z i = d 1 ( i ) v 1 + + d n ( i ) v n , i = 1 , 2 , , k . Thus, we obtain

j 1 = 0 t 1 j n = 0 t n η ( j 1 b 1 u 1 + + j n b n u n + d 1 ) η ( j 1 b 1 u 1 + + j n b n u n + d k ) = j 1 = 0 t 1 j n = 0 t n η j 1 b 1 + d 1 ( 1 ) , , j n b n + d n ( 1 ) η j 1 b 1 + d 1 ( k ) , , j n b n + d n ( k ) = z B i = 1 k 2 d χ i G j i = 0 d 2 1 χ i ( α j i ) χ i ¯ ( f ( z + z i ) ) = 2 k d k χ 1 G j 1 = 0 d 2 1 χ 1 ( α j 1 ) χ k G j k = 0 d 2 1 χ k ( α j k ) z B χ 1 ¯ ( f ( z + z 1 ) ) χ k ¯ ( f ( z + z k ) ) .

Let χ be a generator of the group of multiplicative characters on F q . For u = 1 , , k , we define δ u by χ u ¯ = χ δ u , where 0 < δ u < q 1 . By Lemmas 2.3 and 2.4 we have

z B χ 1 ¯ ( f ( z + z 1 ) ) χ k ¯ ( f ( z + z k ) ) = z B χ ( f δ 1 ( z + z 1 ) f δ k ( z + z k ) ) < k deg ( f ) q 1 2 ( 1 + log p ) n .

Then

j 1 = 0 t 1 j n = 0 t n η ( j 1 b 1 u 1 + + j n b n u n + d 1 ) η ( j 1 b 1 u 1 + + j n b n u n + d k ) < 2 k d k χ G j = 0 d 2 1 χ ( α j ) k k deg ( f ) q 1 2 ( 1 + log p ) n < k 2 2 k deg ( f ) q 1 2 ( 1 + log p ) n log k ( 1 + d )

by Lemma 2.5. It follows that

k ( η ) < k 2 2 k deg ( f ) q 1 2 ( 1 + log p ) n log k ( 1 + d ) ,

which proves Theorem 1.1.

4 Family complexity

We will adopt the methods used in [15, 16] to prove Theorem 1.2. We shall show that for any specification of length K

(4.1) η ( x 1 ) = ε 1 , η ( x 2 ) = ε 2 , , η ( x K ) = ε K ,

where x 1 , x 2 , , x K F p n are K distinct vectors, there is an f S so that the binary lattice η = η f satisfies the specification (4.1).

Note that K < q , thus there is an integer K + 1 satisfying

1 < K + 1 q , x K + 1 { x 1 , x 2 , , x K } .

Let

ε K + 1 = ε 1 ,

and let φ : F p n F q be a mapping defined by

φ ( x ) = φ ( ( x 1 , , x n ) ) = x 1 v 1 + + x n v n F q ,

where x = ( x 1 , , x n ) F p n , and let φ ( x i ) = t i F q for i = 1 , 2 , , K + 1 .

For i = 1 , 2 , , K + 1 , we define

(4.2) y i j = 0 d 2 1 C j ( d , q ) , if ε i = + 1 , j = d 2 d 1 C j ( d , q ) , if ε i = 1 .

It is well known that

(4.3) g ( x ) = i = 1 K + 1 y i L i ( x ) , L i ( x ) = j = 1 j i K + 1 x t j t i t j , i = 1 , , K + 1 ,

is a representation of the unique interpolating polynomial g ( x ) F q [ x ] with deg ( g ) = K corresponding to the data ( t i , y i ) , t i t j for i j , i , j = 1 , , K + 1 .

Note that g ( x ) F q [ x ] with deg ( g ) = K 1 is a non-zero polynomial, by Lemma 2.6, g ( x ) can be written in the form

g ( x ) = ( h ( x ) ) d g ( x ) ,

where h ( x ) , g ( x ) F q [ x ] and the multiplicity of each zero of g ( x ) in F ¯ q is less than d. Let

f ( x ) = g ( x ) .

It follows that

deg ( f ) = deg ( g ) deg ( g ) = K .

By (4.2) and (4.3), we have

(4.4) g ( t i ) = y i j = 0 d 2 1 C j ( d , q ) , if ε i = + 1 , j = d 2 d 1 C j ( d , q ) , if ε i = 1 ,

where i = 1 , 2 , , K + 1 . Therefore,

( h ( t i ) ) d g ( t i ) = g ( t i ) = y i F q ,

and thus

f ( t i ) = g ( t i ) F q .

Then by (3.1) and (4.2) we have

η ( x i ) = 2 d j = 0 d 2 1 χ G χ ¯ ( f ( t i ) ) χ ( α j ) = 2 d j = 0 d 2 1 χ G χ ¯ ( g ( t i ) ) χ ( α j ) = 2 d j = 0 d 2 1 χ G χ ¯ ( ( h ( t i ) ) d g ( t i ) ) χ ( α j ) = 2 d j = 0 d 2 1 χ G χ ¯ ( g ( t i ) ) χ ( α j ) = 2 d j = 0 d 2 1 χ G χ ¯ ( y i ) χ ( α j ) = + 1 , if ε i = + 1 , 1 , if ε i = 1 ,

where i = 1 , 2 , , K + 1 , which implies that

χ ¯ ( f ( t 1 ) ) χ ¯ ( f ( t K + 1 ) ) ,

and deg ( f ) > 0 , and thus f S and the binary lattice η = η f satisfies the specification (4.1). This completes the proof of Theorem 1.2.

5 Collision and avalanche effect

Now we study collision and avalanche effect of the family of binary lattices defined in Theorem 1.3. Suppose that f , g S and f g . By the definition of the distance d ( η f , η g ) between η f and η g , we have

(5.1) d ( η f , η g ) = | { x F p n : η f ( x ) η g ( x ) } | = x F p n 1 2 ( 1 η f ( x ) η g ( x ) ) .

The last part of the sum in Eq. (5.1) can be written as:

x 1 = 0 p 1 x n = 0 p 1 η f ( x 1 , , x n ) η g ( x 1 , , x n ) z F q f ( z ) g ( z ) 0 2 d j 1 = 0 d 2 1 χ 1 G χ 1 ¯ ( f ( z ) ) χ 1 ( α j 1 ) 2 d j 2 = 0 d 2 1 χ 2 G χ 2 ¯ ( g ( z ) ) χ 2 ( α j 2 ) + 2 L = 4 d 2 χ 1 G j 1 = 0 d 2 1 χ 1 ( α j 1 ) χ 2 G j 2 = 0 d 2 1 χ 2 ( α j 2 ) z F q f ( z ) g ( z ) 0 χ 1 ¯ ( f ( z ) ) χ 2 ¯ ( g ( z ) ) + 2 L = 4 d 2 χ 1 G j 1 = 0 d 2 1 χ 1 ( α j 1 ) χ 2 G j 2 = 0 d 2 1 χ 2 ( α j 2 ) z F q χ 1 ¯ ( f ( z ) ) χ 2 ¯ ( g ( z ) ) + 2 L .

Let χ be a generator of the group of multiplicative characters on F q . Define χ 1 ¯ = χ δ 1 and χ 2 ¯ = χ δ 2 , where 0 < δ 1 , δ 2 < q 1 . Note that f , g S , f g and f , g have no multiple zero in F ¯ q , thus f δ 1 g δ 2 is not a constant times of a ( q 1 ) th power of a polynomial. Applying Lemma 2.2 we obtain

z F q χ 1 ¯ ( f ( z ) ) χ 2 ¯ ( g ( z ) ) = z F q χ ( f δ 1 ( z ) g δ 2 ( z ) ) ( 2 L 1 ) q 1 2 .

Then

x F p n η f ( x ) η g ( x ) 4 d 2 χ G j = 0 d 2 1 χ ( α j ) 2 ( 2 L 1 ) q 1 2 < 16 ( 2 L 1 ) q 1 2 log 2 ( 1 + d ) .

It follows that

d ( η f , η g ) q 2 8 ( 2 L 1 ) q 1 2 log 2 ( 1 + d ) L

and

m ( ) = min f , g S f g d ( η f , η g ) q 2 8 ( 2 L 1 ) q 1 2 log 2 ( 1 + d ) L ,

which proves Theorem 1.3.

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Received: 2019-11-22
Revised: 2020-07-21
Accepted: 2020-09-10
Published Online: 2020-12-29

© 2020 Xiaolin Chen, published by De Gruyter

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

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  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
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