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BY 4.0 license Open Access Published by De Gruyter Open Access May 14, 2021

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
From the journal Open Mathematics

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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