Home Multiple solutions and ground state solutions for a class of generalized Kadomtsev-Petviashvili equation
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Multiple solutions and ground state solutions for a class of generalized Kadomtsev-Petviashvili equation

  • Yuting Zhu , Chunfang Chen EMAIL logo , Jianhua Chen and Chenggui Yuan
Published/Copyright: May 14, 2021

Abstract

In this paper, we study the following generalized Kadomtsev-Petviashvili equation

u t + u x x x + ( h ( u ) ) x = D x 1 Δ y u ,

where ( t , x , y ) R + × R × R N 1 , N 2 , D x 1 f ( x , y ) = x f ( s , y ) d s , f t = f t , f x = f x and Δ y = i = 1 N 1 2 y i 2 . We get the existence of infinitely many nontrivial solutions under certain assumptions in bounded domain without Ambrosetti-Rabinowitz condition. Moreover, by using the method developed by Jeanjean [13], we establish the existence of ground state solutions in R N .

MSC 2010: 35J60; 35J20

1 Introduction

This article is concerned with the following generalized Kadomtsev-Petviashvili equation:

(1.1) u t + u x x x + ( h ( u ) ) x = D x 1 Δ y u ,

where ( t , x , y ) R + × R × R N 1 , N 2 , D x 1 f ( x , y ) = x f ( s , y ) d s , f t = f t , f x = f x and Δ y = i = 1 N 1 2 y i 2 .

To find a solitary wave for (1.1), it needs us to get a solution u of the form u ( t , x , y ) = u ( x τ t , y ) , with τ 0 . Hence, equation (1.1) can be rewritten as:

(1.2) τ u x + u x x x + ( h ( u ) ) x = D x 1 Δ y u in R N .

If we choose h ( s ) = s 2 in (1.1), then equation (1.1) is a two-dimensional generalization of the Korteweg-de Vries equation, which describes long dispersive waves in mathematical models, see [1]. When h ( s ) = s p s with p = m n , where m and n are relative prime numbers, and n is odd, Bouard and Saut [2,3] proved that there is a solitary wave for (1.1) with 1 p < 4 , if N = 2 , or 1 p < 4 3 , if N = 3 , via the concentration compactness principle from [4,5]. In [6], Willem proved the existence of solitary waves of (1.1) as N = 2 and h C 1 ( R , R ) . In [7], Xuan extended the results obtained by [6] to higher dimension. In [8], h ( u ) was replaced by Q ( x , y ) u p 2 u , and Liang and Su had obtained nontrivial solutions of (1.1). In [9], Xu and Wei studied infinitely many solutions for u x x x + ( h ( u ) ) x = D x 1 Δ y u with the Ambrosetti-Rabinowitz condition in bounded domain. For related contributions to study of solitary waves of the generalized Kadomtsev-Petviashvili equations, we refer to previous studies [10,11].

The aim of this paper is to prove the existence of multiple solutions of (1.3) in bounded domain without condition (AR), which is to ensure the boundedness of the (PS) sequences of the corresponding functional, and obtain the ground state solutions of (1.2) in R N . In what follows, we assume that the function h : R R satisfies the following conditions:

  1. h C ( R ) , h ( 0 ) = 0 ;

  2. for some p ( 1 , N ¯ 1 ) , where N ¯ = 4 N 2 2 N 3 , lim t + h ( t ) t p = lim t 0 h ( t ) t = 0 ;

  3. h ( t ) = h ( t ) , lim t + H ( t ) t 2 = + , where H ( t ) = 0 t h ( r ) d r ;

  4. there exist μ > 2 , κ > 0 such that μ H ( t ) t h ( t ) + κ t 2 ;

  5. there exists μ > 2 such that 0 μ H ( t ) h ( t ) t .

Consider the following system,

(1.3) τ u x + u x x x + ( h ( u ) ) x = D x 1 Δ y u , in Ω , u = 0 , on Ω ,

where Ω R N is a bounded domain.

Now, we can state our first result.

Theorem 1.1

Assume that ( h 1 ) ( h 4 ) are satisfied, then equation (1.3) possesses infinitely many nontrivial solutions in Ω , where Ω R N is a bounded domain.

Our second result is as follows.

Theorem 1.2

Assume that ( h 1 ) ( h 2 ) and ( h 5 ) are satisfied, then equation (1.2) has a ground state solution.

Notations. Throughout the paper, we denote by p the usual norm of Lebesgue space L p ( R N ) . X is the dual space of X . The symbol C denotes a positive constant and may vary from line to line.

2 Preliminary

In this section, we want to introduce the functional setting and some main results. At first, we present the functional setting (see [7,11]).

Definition 2.1

[7] On Y = g x : g C 0 R N , define the inner product

( u , v ) = R N u x v x + D x 1 y u D x 1 y v + τ u v d V , τ > 0 ,

and the norm is

u = R N u x 2 + D x 1 y u 2 + τ u 2 d V 1 2 , τ > 0

where y = y 1 , , y N 1 and d V = d x d x .

If there exists a sequence u n Y such that u n u a.e. on R N , and u j u k 0 as j , k , then we say that u : R N R belongs to X .

Definition 2.2

[7] On Y = g x : g C 0 R N , define the inner product

( u , v ) 0 = R N u x v x + D x 1 y u D x 1 y v d V ,

and the norm is

u 0 = R N u x 2 + D x 1 y u 2 d V 1 2 ,

where y = y 1 , , y N 1 and d V = d x d x .

If there exists a sequence u n Y such that u n u a.e. on R N , and u j u k 0 0 as j , k , then we say that u : R N R belongs to X 0 .

Lemma 2.1

[7,11,12] The following continuous embeddings hold.

  1. the embeddings X X 0 are continuous;

  2. the embeddings X L q R N , for 1 q N ¯ are continuous;

  3. the embeddings X L loc q R N , for 1 q < N ¯ are compact;

  4. the embeddings X 0 L N ¯ R N are continuous.

Lemma 2.2

[14] Let X be an infinite dimensional Banach space, and there exists a finite dimensional space W such that X = W V . I C 1 ( R ) satisfies the ( P S ) condition, and

  1. I ( u ) = I ( u ) for all u X , I ( 0 ) = 0 ;

  2. there exist ρ > 0 , α > 0 such that I B ρ V α ;

  3. for any finite dimensional subspace Y X , there is R = R ( Y ) > 0 such that I ( u ) 0 on Y \ B R .

Then I possesses an unbounded sequence of critical values.

Lemma 2.3

[7] Assume that u n is a bounded sequence in X . If

lim n + sup ( x , y ) R N B r ( ( x , y ) ) u n 2 d V = 0 ,

then u n 0 in L q R N for all q ( 2 , N ¯ ) .

Lemma 2.4

[13] Let ( X , ) be a Banach space and T R + be an interval. Consider a family of C 1 functionals on X of the form

I λ ( u ) = A ( u ) λ B ( u ) λ T ,

with B ( u ) 0 and either A ( u ) + or B ( u ) + as u + . If there are two points v 1 , v 2 X such that

c λ = inf γ Γ max t [ 0 , 1 ] I λ ( γ ( t ) ) > max I λ v 1 , I λ v 2 λ T ,

where

Γ = γ C ( [ 0 , 1 ] , X ) : γ ( 0 ) = v 1 , γ ( 1 ) = v 2 .

Then, for almost every λ T , there exists a bounded ( P S ) c λ sequence in X , and the mapping λ c λ is non-increasing and left continuous.

3 Proof of Theorem 1.1

In this section, we consider the boundary value problem (1.3). The energy functional I : X R given by

I ( u ) = 1 2 u 2 R N H ( u ) d V

and

I ( u ) [ v ] = R N u x v x + D x 1 y u D x 1 y v + τ u v d V R N h ( u ) v d V .

Lemma 3.1

Suppose h satisfies h 1 h 4 . If u n X satisfies

  1. I u n is bounded;

  2. I u n , u n 0 ,

then u n is bounded in X .

Proof

If u n is unbounded in X , we can find a subsequence still denoted by u n such that u n + . Let v n = u n u n , we have v n = 1 . Thus, we may assume that v n v in X . As the embedding X L loc 2 R N is compact, we have v n v in L 2 ( Ω ) . By h 4 and ( i ) , there exists c > 0 such that

c + 1 I u n 1 μ I u n , u n μ 2 2 μ u n 2 κ μ u n 2 2 = μ 2 2 μ u n 2 v n 2 κ μ u n 2 v n 2 2 ,

as n + , which implies 1 2 κ μ 2 lim n + sup v n 2 2 . Therefore, v 0 . By h 3 and Fatou’s Lemma, one has

0 = lim n + c u n 2 = lim n + I u n u n 2 = lim n + 1 2 R N H ( u ) u n 2 v n 2 = ,

which is a contradiction. Hence, u n is bounded in X .□

Lemma 3.2

Suppose h satisfies ( h 1 ) ( h 4 ) . Then the functional I satisfies the (PS) condition.

Proof

To prove that I satisfies the (PS) condition, we only need to prove { u n } X has a convergent subsequence, where { u n } obtained by Lemma 3.1. As { u n } is bounded in X , there exists a subsequence still denoted by { u n } and u 0 X such that u n u 0 in X and u n u 0 in L q ( Ω ) for 1 q < N ¯ . From ( h 2 ) , we have

h ( u n ) ε u n + C ε u n p , ε > 0 .

then

R N h ( u n ) p + 1 p d V p p + 1 R N ε u n + C ε u n p p + 1 p d V p p + 1 C u n + u n p < + .

Applying the Hölder inequality, for 1 < p < N ¯ 1 , one has

Ω h u n h u 0 u n u 0 d V Ω h u n h u 0 p + 1 p d V p p + 1 Ω u n u 0 p + 1 d V 1 p + 1 C Ω ( h u n p + 1 p + h u 0 p + 1 p ) d V p p + 1 Ω u n u 0 p + 1 d V 1 p + 1 0 .

It follows from u n u 0 in X and I ( u 0 ) X * that I u 0 , u n u 0 0 . And as I ( u n ) 0 in X , it is easy to obtain

I ( u n ) , u n u 0 I ( u n ) X u n u 0 X ( Ω ) 0 .

Therefore,

I u n I ( u 0 ) , u n u 0 = I ( u 0 ) , u n u 0 I ( u n ) , u n u 0 0 ,

as n + .

Thus, we have

u n u 0 2 = I u n I ( u ) , u n u + Ω h u n h u 0 u n u 0 d V 0 ,

as n + .□

Proof

Proof of Theorem 1.1. We have verified that I satisfies the (PS) condition. It follows from ( h 5 ) that I is an even function. As X is a separable space, X has orthonormal basis { e i } . Define X j R e j , W k j = 1 k X j , V k j = k + 1 X j ¯ . Let W = W k , V = V k , clearly X = W V and dim W < .

Next, we verify that I satisfies (ii) in Lemmas 2.2. By Lemma 2.1, for all u V , we have

I ( u ) = 1 2 u 2 R N H ( u ) d V 1 2 u 2 ε 2 u 2 2 + C ε p u p + 1 p + 1 1 2 u 2 C ε u 2 + C ε u p + 1 .

Then there exists ρ > 0 small enough, α > 0 such that I ( u ) α > 0 as u = ρ .

Now, we verify that I satisfies (iii) in Lemma 2.2. For any finite dimensional subspace Y X , since lim t + H ( t ) t 2 = + , for u 0 ,

I r u = r 2 2 u 2 R N H r u d V = r 2 2 u 2 2 R N H r u r u 2 u 2 d V ,

as r + . Thus, there exists r 0 > 0 such that I r u < 0 for all r r 0 > 0 . So we can conclude that there exists a R ( Y ) > 0 such that I ( u ) 0 on Y \ B R ( Y ) .

Hence, according to Lemma 2.2, equation (1.3) possesses infinitely many nontrivial solutions.□

4 Proof of Theorem 1.2

In this section, the weak solutions of (1.2) are the critical points of the energy functional I , where I ( u ) = 1 2 u 2 R N H ( u ) d V . As h satisfies h 1 h 2 and h 5 , it is clear that I is of class C 1 ( X , R ) . To apply Jeanjean’s trick [ 13 ] , we give a family of energy functions

I λ ( u ) = 1 2 u 2 λ R N H ( u ) d V , λ 1 2 , 1 .

Lemma 4.1

Suppose that h satisfies ( h 1 ) ( h 2 ) and ( h 5 ) . Then

  1. there exists v X { 0 } such that I λ ( v ) < 0 for all λ 1 2 , 1 ;

  2. c λ = inf γ Γ max t [ 0 , 1 ] I λ ( γ ( t ) ) > max I λ ( 0 ) , I λ ( v ) for all λ 1 2 , 1 , where

Γ = { γ C ( [ 0 , 1 ] , X ) : γ ( 0 ) = 0 , γ ( 1 ) = v } .

Proof

(i) By ( h 5 ) , we have lim s + H ( s ) s 2 = + . Furthermore, for some u X

I λ ( t u ) = t 2 2 u 2 λ R N H ( t u ) d V t 2 2 u 2 R N H ( t u ) ( t u ) 2 u 2 d V as t + .

Thus, there exists t 0 > 0 such that I λ t 0 u < 0 . By taking v = t 0 u , we have I λ ( v ) < 0 .

(ii) By virtue of ( h 2 ) , for any ε > 0 and some p ( 1 , N ¯ 1 ) , there exists C ε > 0 such that

H ( t ) ε 2 t 2 + C ε p t p + 1 t R .

By Lemma 2.1, we have

I λ ( u ) = 1 2 u 2 λ R N H ( u ) d V 1 2 u 2 ε 2 u 2 2 + C ε p u p + 1 p + 1 1 2 u 2 C ε u 2 + C ε u p + 1 .

Then there exists ρ > 0 small enough such that

b inf u = ρ I λ ( u ) > 0 = I λ ( 0 ) > I λ ( v ) .

Therefore, c λ > max I λ ( 0 ) , I λ ( v ) .□

Combining Lemma 4.1 with Theorem 2.6, we have the following conclusion.

Lemma 4.2

Suppose h satisfies ( h 1 ) ( h 2 ) and ( h 5 ) . For almost every λ 1 2 , 1 , there is a bounded sequence { v m } , such that I λ ( v m ) c λ in X and I λ ( v m ) 0 in the dual X of X .

Lemma 4.3

If v m is a bounded sequence in X and lim m + sup ( x , y ) R N B 1 ( ( x , y ) ) v m 2 d V = 0 , then lim m + R N G v m = 0 , where G v m = 1 2 h v m v m H v m .

Proof

On one hand, by simple calculations, we derive

R N H v m d V ε 2 v m 2 2 + C ε p + 1 v m p + 1 p + 1 ,

R N h v m v m d V ε v m 2 2 + C ε v m p + 1 p + 1 .

On the other hand, by Lemma 2.3, we have v m 0 in L q ( R N ) for all q ( 2 , N ¯ ) . Hence, we can conclude that

lim m + R N H v m d V = 0 ,

lim m + R N h v m v m d V = 0 .

Thus, lim m + R N G v m d V = 0 .□

Lemma 4.4

If v m X is the sequence obtained by Lemma 4.2, then for a.e. λ 1 2 , 1 , there exists a sequence of points x m , y m R × R N 1 , u m ( x , y ) v m x x m , y y m , such that

  1. u m u λ 0 in X ;

  2. I λ u λ = 0 in X * ;

  3. I λ u λ c λ in X ; and

  4. there exists M > 0 such that I λ u λ M .

Proof

By Lemma 4.2, we know that for almost every λ 1 2 , 1 , there exists a bounded sequence v m that satisfy I λ v m c λ in X and I λ v m 0 in X * as m + . Furthermore,

R N G v m = I λ v m 1 2 I λ v m , v m c λ > 0 as m + .

By Lemma 4.3, there exist a sequence of points x m , y m R × R N 1 and α > 0 , such that

B 1 x m , y m v m 2 d V α > 0 .

Let u m ( x , y ) v m x x m , y y m . By the invariance translations of I λ , as m + , we have that I λ u m c λ in X and I λ u m 0 in X * . Since u m is bounded, there exists u λ X such that u m u λ in X .

In the following, we complete the proof of this lemma.

  1. It follows from Lemma 2.1 that

    C u λ 2 u λ 2 2 B 1 ( 0 ) u λ 2 d V = lim m + B 1 ( 0 ) u m 2 d V α > 0 ,

    and thus obtain u λ 0 in X .

  2. As C 0 R N is dense in X , we only need to check that I λ u λ , φ = 0 for any φ X . We have

    I λ u m , φ I λ u λ , φ = u m u λ , φ λ R N h u m h u λ φ d V 0 ,

    since u m u λ in X , u m u λ in L loc p R N for 1 p N ¯ . It follows from I λ u m 0 that I λ u λ = 0 .

  3. By ( h 5 ) and Fatou’s Lemma, we get

    c λ = lim m + I λ u m 1 2 I λ u m , u m = λ lim m + R N G u m d V λ R N G u λ d V = I λ u λ 1 2 I λ u λ , u λ = I λ u λ .

  4. Combining (ii) with h 2 and Lemma 2.1, we obtain that for any ε > 0 , there exists C ε > 0 such that

    u λ 2 = λ R N h u λ u λ d V R N h u λ u λ d V C ε u λ 2 + C ε u λ p + 1 .

    Then there exists β > 0 such that u λ β > 0 . Therefore,

    I λ u λ = I λ u λ 1 μ I λ u λ , u λ = 1 2 1 μ u λ 2 + R N 1 μ h u λ u λ H u λ d V 1 2 1 μ u λ 2 1 2 1 μ β 2 M > 0 .

This completes the proof.□

Now, according to Lemmas 4.2 and 4.4, there exists a sequence λ n , u λ n 1 2 , 1 × X , such that

(i) λ n 1 as n + ; (ii) u λ n 0 , M I λ n u λ n c λ n and I λ n u λ n = 0 .

Lemma 4.5

(Pohozaev identity, [7]) Suppose h satisfies h 1 h 2 . If u X is a weak solution of the equation:

τ u x + u x x x + λ ( h ( u ) ) x = D x 1 Δ y u in R N ,

then we have the following Pohozaev identity:

P λ ( u ) 2 N 3 2 u 0 2 + ( 2 N 1 ) R N τ 2 u 2 λ H ( u ) d V = 0 .

Proof

Proof of Theorem 1.2. By Lemma 4.5, if u λ n is nontrivial solution of equation

τ u x + u x x x + λ n ( h ( u ) ) x = D x 1 Δ y u in R N ,

then u λ n satisfies the following equation:

P λ n u λ n = 2 N 3 2 u λ n 0 2 + ( 2 N 1 ) τ 2 R N u λ n 2 d V ( 2 N 1 ) λ n R N H u λ n d V = 0 .

Remember that

c λ n I λ n u λ n 1 2 N 1 P λ n u λ n = 1 2 N 1 u λ n 0 2 .

So,

u λ n 0 2 ( 2 N 1 ) c λ n ( 2 N 1 ) c 1 2 ,

it follows from Lemma 2.1 that u λ n is bounded in X 0 and also in L N ¯ .

Since I λ n u λ n = 0 , we have

I λ n u λ n , u λ n = u λ n 2 λ n R N h u λ n u λ n d V = 0 .

Moreover, by Lemma 2.1, for any ε > 0 , there exists C ε > 0 such that

u λ n 2 = λ n R N h u λ n u λ n d V ε C u λ n 2 + C ε u λ n N ¯ N ¯ .

Then, for ε small enough, there exists a constant C > 0 such that u λ n 2 C , since u λ n is bounded in L N ¯ . Thus, u λ n is bounded in X . By the facts that for any φ X ,

I u λ n , φ = I λ n u λ n , φ + λ n 1 R N h u λ n φ d V ,

I u λ n = I λ n u λ n + λ n 1 R N H u λ n d V ,

and u λ n is bounded in X , it follows that M lim n + I u λ n c 1 and lim n + I u λ n = 0 . Up to a subsequence, there exists a subsequence still denoted by u λ n and u 0 X such that u λ n u 0 in X . By using the method in Lemma 4.4, we can obtain the existence of a nontrivial solution u 0 for I such that I u 0 = 0 and I u 0 c 1 . Thus, u 0 is a nontrivial solution of (1.2). Define m inf I ( u ) : u 0 , I ( u ) = 0 . Let u n be a sequence such that I u n = 0 and I u n m . Similar to arguments in Lemma 4.4, we can prove that there exists u ¯ X such that I ( u ¯ ) = 0 and I ( u ¯ ) m . By the definition of m , we have m I ( u ¯ ) . Hence, I ¯ ( u ¯ ) = m , which shows that u ¯ is a ground state solution of (1.2).□

Acknowledgements

This work was supported by the National Natural Science Foundation of China (Grant Nos. 11661053, 11771198, 11901276 and 11961045) and the Provincial Natural Science Foundation of Jiangxi, China (20181BAB201003, 20202BAB201001 and 20202BAB211004).

  1. Conflict of interest: The authors declare that they have no competing interests.

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Received: 2020-06-23
Accepted: 2021-01-09
Published Online: 2021-05-14

© 2021 Yuting Zhu et al., published by De Gruyter

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

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  52. Refinements of quantum Hermite-Hadamard-type inequalities
  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
  56. Several explicit formulas for (degenerate) Narumi and Cauchy polynomials and numbers
  57. Finite groups whose intersection power graphs are toroidal and projective-planar
  58. On primitive solutions of the Diophantine equation x2 + y2 = M
  59. A note on polyexponential and unipoly Bernoulli polynomials of the second kind
  60. On the type 2 poly-Bernoulli polynomials associated with umbral calculus
  61. Some estimates for commutators of Littlewood-Paley g-functions
  62. Construction of a family of non-stationary combined ternary subdivision schemes reproducing exponential polynomials
  63. On the evolutionary bifurcation curves for the one-dimensional prescribed mean curvature equation with logistic type
  64. On intersections of two non-incident subgroups of finite p-groups
  65. Global existence and boundedness in a two-species chemotaxis system with nonlinear diffusion
  66. Finite groups with 4p2q elements of maximal order
  67. Positive solutions of a discrete nonlinear third-order three-point eigenvalue problem with sign-changing Green's function
  68. Power moments of automorphic L-functions related to Maass forms for SL3(ℤ)
  69. Entire solutions for several general quadratic trinomial differential difference equations
  70. Strong consistency of regression function estimator with martingale difference errors
  71. Fractional Hermite-Hadamard-type inequalities for interval-valued co-ordinated convex functions
  72. Montgomery identity and Ostrowski-type inequalities via quantum calculus
  73. Universal inequalities of the poly-drifting Laplacian on smooth metric measure spaces
  74. On reducible non-Weierstrass semigroups
  75. so-metrizable spaces and images of metric spaces
  76. Some new parameterized inequalities for co-ordinated convex functions involving generalized fractional integrals
  77. The concept of cone b-Banach space and fixed point theorems
  78. Complete consistency for the estimator of nonparametric regression model based on m-END errors
  79. A posteriori error estimates based on superconvergence of FEM for fractional evolution equations
  80. Solution of integral equations via coupled fixed point theorems in 𝔉-complete metric spaces
  81. Symmetric pairs and pseudosymmetry of Θ-Yetter-Drinfeld categories for Hom-Hopf algebras
  82. A new characterization of the automorphism groups of Mathieu groups
  83. The role of w-tilting modules in relative Gorenstein (co)homology
  84. Primitive and decomposable elements in homology of ΩΣℂP
  85. The G-sequence shadowing property and G-equicontinuity of the inverse limit spaces under group action
  86. Classification of f-biharmonic submanifolds in Lorentz space forms
  87. Some new results on the weaving of K-g-frames in Hilbert spaces
  88. Matrix representation of a cross product and related curl-based differential operators in all space dimensions
  89. Global optimization and applications to a variational inequality problem
  90. Functional equations related to higher derivations in semiprime rings
  91. A partial order on transformation semigroups with restricted range that preserve double direction equivalence
  92. On multi-step methods for singular fractional q-integro-differential equations
  93. Compact perturbations of operators with property (t)
  94. Entire solutions for several complex partial differential-difference equations of Fermat type in ℂ2
  95. Random attractors for stochastic plate equations with memory in unbounded domains
  96. On the convergence of two-step modulus-based matrix splitting iteration method
  97. On the separation method in stochastic reconstruction problem
  98. Robust estimation for partial functional linear regression models based on FPCA and weighted composite quantile regression
  99. Structure of coincidence isometry groups
  100. Sharp function estimates and boundedness for Toeplitz-type operators associated with general fractional integral operators
  101. Oscillatory hyper-Hilbert transform on Wiener amalgam spaces
  102. Euler-type sums involving multiple harmonic sums and binomial coefficients
  103. Poly-falling factorial sequences and poly-rising factorial sequences
  104. Geometric approximations to transition densities of Jump-type Markov processes
  105. Multiple solutions for a quasilinear Choquard equation with critical nonlinearity
  106. Bifurcations and exact traveling wave solutions for the regularized Schamel equation
  107. Almost factorizable weakly type B semigroups
  108. The finite spectrum of Sturm-Liouville problems with n transmission conditions and quadratic eigenparameter-dependent boundary conditions
  109. Ground state sign-changing solutions for a class of quasilinear Schrödinger equations
  110. Epi-quasi normality
  111. Derivative and higher-order Cauchy integral formula of matrix functions
  112. Commutators of multilinear strongly singular integrals on nonhomogeneous metric measure spaces
  113. Solutions to a multi-phase model of sea ice growth
  114. Existence and simulation of positive solutions for m-point fractional differential equations with derivative terms
  115. Bernstein-Walsh type inequalities for derivatives of algebraic polynomials in quasidisks
  116. Review Article
  117. Semiprimeness of semigroup algebras
  118. Special Issue on Problems, Methods and Applications of Nonlinear Analysis (Part II)
  119. Third-order differential equations with three-point boundary conditions
  120. Fractional calculus, zeta functions and Shannon entropy
  121. Uniqueness of positive solutions for boundary value problems associated with indefinite ϕ-Laplacian-type equations
  122. Synchronization of Caputo fractional neural networks with bounded time variable delays
  123. On quasilinear elliptic problems with finite or infinite potential wells
  124. Deterministic and random approximation by the combination of algebraic polynomials and trigonometric polynomials
  125. On a fractional Schrödinger-Poisson system with strong singularity
  126. Parabolic inequalities in Orlicz spaces with data in L1
  127. Special Issue on Evolution Equations, Theory and Applications (Part II)
  128. Impulsive Caputo-Fabrizio fractional differential equations in b-metric spaces
  129. Existence of a solution of Hilfer fractional hybrid problems via new Krasnoselskii-type fixed point theorems
  130. On a nonlinear system of Riemann-Liouville fractional differential equations with semi-coupled integro-multipoint boundary conditions
  131. Blow-up results of the positive solution for a class of degenerate parabolic equations
  132. Long time decay for 3D Navier-Stokes equations in Fourier-Lei-Lin spaces
  133. On the extinction problem for a p-Laplacian equation with a nonlinear gradient source
  134. General decay rate for a viscoelastic wave equation with distributed delay and Balakrishnan-Taylor damping
  135. On hyponormality on a weighted annulus
  136. Exponential stability of Timoshenko system in thermoelasticity of second sound with a memory and distributed delay term
  137. Convergence results on Picard-Krasnoselskii hybrid iterative process in CAT(0) spaces
  138. Special Issue on Boundary Value Problems and their Applications on Biosciences and Engineering (Part I)
  139. Marangoni convection in layers of water-based nanofluids under the effect of rotation
  140. A transient analysis to the M(τ)/M(τ)/k queue with time-dependent parameters
  141. Existence of random attractors and the upper semicontinuity for small random perturbations of 2D Navier-Stokes equations with linear damping
  142. Degenerate binomial and Poisson random variables associated with degenerate Lah-Bell polynomials
  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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