Home Mathematics Ground state solution for some new Kirchhoff-type equations with Hartree-type nonlinearities and critical or supercritical growth
Article Open Access

Ground state solution for some new Kirchhoff-type equations with Hartree-type nonlinearities and critical or supercritical growth

  • Li Zhou and Chuanxi Zhu EMAIL logo
Published/Copyright: August 29, 2022

Abstract

In this article, we study two classes of Kirchhoff-type equations as follows:

a + b R 3 u 2 d x Δ u + V ( x ) u = ( I α u p ) u p 2 u + f ( u ) , in R 3 , u H 1 ( R 3 ) ,

and

a + b R 3 u 2 d x Δ u + V ( x ) u = ( I α u p ) u p 2 u + m u l 2 u , in R 3 , u H 1 ( R 3 ) ,

where a > 0 , b 0 , α ( 0 , 3 ) , ( 3 + α ) / 3 < p < ( 3 + α ) , l 6 , m > 0 , V : R 3 R is a potential function and I α is a Riesz potential whose order is α ( 0 , 3 ) . Under some assumptions on V ( x ) and f ( u ) , we can prove that the equations have ground state solutions by variational methods.

MSC 2010: 35J60; 35J35; 35A15

1 Introduction

In this article, we study the following two classes of Kirchhoff-type equations:

(1) a + b R 3 u 2 d x Δ u + V ( x ) u = ( I α u p ) u p 2 u + f ( u ) , in R 3 , u H 1 ( R 3 ) ,

and

(2) a + b R 3 u 2 d x Δ u + V ( x ) u = ( I α u p ) u p 2 u + m u l 2 u , in R 3 , u H 1 ( R 3 ) ,

where a > 0 , b 0 , α ( 0 , 3 ) , ( 3 + α ) / 3 < p < ( 3 + α ) , l 6 , m > 0 , I α is a Riesz potential whose order is α ( 0 , 3 ) . Here, I α = Γ 3 α 2 Γ α 2 π 3 2 2 α x 3 α . Besides, V ( x ) : R 3 R is a potential function satisfying:

  1. V C 1 ( R 3 ) L , and there exists a constant A ( 0 , a ) such that

    ( V ( x ) , x ) A 2 x 2 ,

    for all x R 3 { 0 } ,

  2. there is a constant V > 0 such that for all x R 3 ,

    0 < V ( x ) liminf y + V ( y ) = V < + ,

  3. inf x R 3 V ( x ) V 0 > 0 .

Furthermore, we suppose that the function f C 1 ( R , R ) satisfies:
  1. there exists a constant C 0 > 0 and q ( 2 , 6 ) such that f ( t ) C 0 ( 1 + t q 1 ) , t R ,

  2. f ( t ) = o ( t ) as t 0 ,

  3. lim t + F ( t ) t 2 = , where F ( t ) = 0 t f ( s ) d s ,

  4. f ( t ) t is increasing on ( , 0 ) ( 0 , + ) .

In the past decades, many scholars have studied the existence of nontrivial solutions for the Kirchhoff-type problem:

(3) a + b R 3 u 2 d x Δ u + V ( x ) u = g ( x , u ) , in R 3 , u H 1 ( R 3 ) ,

where a > 0 , b 0 , V : R 3 R is a potential function and g C ( R 3 × R , R ) . Problem (3) is a nonlocal problem because of the presence of the term b R 3 u 2 d x , which causes some mathematical difficulties, but at the same time makes the research of this problem particularly interesting. Besides, this problem has an interesting physical context. In fact, if we set V ( x ) = 0 and replace R 3 by a bounded domain Ω R 3 in (3), then we obtain the following Kirchhoff Dirichlet problem:

a + b Ω u 2 d x Δ u = g ( x , u ) , x Ω , u = 0 , x Ω .

It has relation to the stationary analogue of the equation:

ρ 2 u t 2 ρ 0 h + E 2 L 0 L u x d x 2 u x 2 = 0 ,

which was proposed by G. Kirchhoff as an extension of classical D’Alemberts wave equations for free vibration of elastic strings. Kirchhoff’s model considers the changes in length of the string, which were produced by transverse vibrations. Then J. L. Lions finished the previous work. He introduced a functional analysis approach. After that, more and more researchers have paid much attention to the problem (3). But most of their results need to assume:

  1. V verifies (V): inf x R 3 V ( x ) V 0 > 0 and for each M > 0 .

    meas { x R N : V ( x ) M } < + ,

  2. g satisfies classical Ambrosetti-Rabinowitz condition, i.e., ( A R ) condition: there exists μ > 2 such that

    0 < μ G ( x , s ) s g ( x , s )

    for all s > 0 .

In fact, (V) is sufficient to ensure that the embedding

u H 1 ( R 3 ) : R 3 V ( x ) u 2 d x < + L p ( R 3 ) , 2 p < 6

is compact.

Unfortunately, there still are very few results of existence of ground state solution to (3) without (A-R) condition (see [1,2,3]).

In [3], Guo studied the following Kirchhoff-type problem:

(4) a + b R 3 u 2 d x Δ u + V ( x ) u = f ( u ) , in R 3 . u H 1 ( R 3 ) .

He proved the existence of positive ground states to (4), and in his paper, he did not use (A-R) type condition. He defined a new manifold:

= u H 1 ( R 3 ) : 1 2 Φ ( u ) , u + P ( u ) = 0 ,

which is named the Nehari-Pohozaev manifold. Here,

Φ ( u ) = 1 2 R 3 [ a u 2 + V u 2 ] d x + b 4 R 3 u 2 d x 2 R 3 F ( u ) d x

and

P ( u ) = 1 2 R 3 [ a u 2 + 3 V u 2 ] d x + b 2 R 3 u 2 d x 2 3 R 3 F ( u ) d x

are the energy functional and Pohozaev identity for the “limit problem” of problem (4), respectively. He first applied the result, which was obtained for the related “limit problem” of (4) to obtain a minimizer for problem (4) on the Nehari-Pohozaev manifold.

We must point out that f C 1 and the fourth assumption about f are very important in Guo [3]. Actually, only under aforementioned assumptions, is a C 1 manifold.

Most remarkably, as early as 2006, Ruiz [4] first proposed the prototype of this Nehari-Pohozaev manifold in his study of the Schrödinger-Poisson equation, which is a very great work.

On the other hand, when a = 1 , b = 0 , f = 0 , equation (1) becomes

(5) Δ u + V ( x ) u = ( I α u p ) u p 2 u .

We usually call it nonlinear Choquard-type equation. Its physical background can be found in [5], and the references therein. Besides, readers can see [6,7,8, 9,10,11, 12,13] for recent achievements.

Inspired by the aforementioned works, especially by [3,13, 14,15], we now research problem (3) with Hartree-type nonlinearities g ( x , u ) = ( I α u p ) u p 2 u + f ( u ) , which may be regarded as a Kirchhoff-type perturbation to (5). As we all know, there are very few results to (3) with Hartree-type nonlinearities and critical or supercritical growth.

The main outcomes of our investigation are as follows.

Theorem 1.1

If V satisfies ( V 1)–( V 2), f C 1 ( R , R ) verifies ( f 1)–( f 4), then problem (1) has a ground state solution.

Theorem 1.2

If V satisfies (V1)–(V3), then there exists some m 0 > 0 such that for m ( 0 , m 0 ] , problem (2) has a ground state solution.

For the convenience of expression, hereafter, we will use the following notations:

  • X H 1 ( R 3 ) is a space in which an equivalent norm is defined as follows:

    u = R 3 ( a u 2 + V ( x ) u 2 ) d x 1 2 ,

  • L s ( R 3 ) ( 1 s ) denotes the Lebesgue space in which the norm is defined as follows:

    u s = R 3 u s d x 1 / s ,

  • For any u H 1 ( R 3 ) { 0 } , u t is denoted as follows:

    u t = 0 , t = 0 , t u x t , t > 0 .

  • For any x R 3 and r > 0 , B r ( x ) { y R 3 : y x < r } .

  • C , C 1 , C 2 , denote positive constants, which are possibly different in different lines.

2 Preliminaries

Problem (1) has a variational structure, i.e., the critical points of the functional

(6) I ( u ) = 1 2 R 3 [ a u 2 + V ( x ) u 2 ] d x + b 4 R 3 u 2 d x 2 1 2 p R 3 ( I α u p ) u p d x R 3 F ( u ) d x

are weak solutions of problem (1).

Lemma 2.1

Assume that ( f 1)–( f 4) hold, then we have

  1. for all ε > 0 and q ( 2 , 6 ) , there is a C ε > 0 such that f ( t ) ε t + C ε t q 1 ,

  2. for any s 0 , s f ( s ) > 2 F ( s ) and F ( s ) > 0 .

Proof

We could easily obtain the results by elementary calculation.□

Lemma 2.2

(Hardy-Littlewood-Sobolev inequality [16]). Let 0 < α < N , p , q > 1 and 1 r < s < be such that

1 p + 1 q = 1 + α N , 1 r 1 s = α N .

  1. For any f L p ( R N ) and g L q ( R N ) , one has

    R N R N f ( x ) g ( y ) x y N α d x d y C ( N , α , p ) f L p ( R N ) g L q ( R N ) .

  2. For any f L r ( R N ) , one has

    1 N α f L s ( R N ) C ( N , α , r ) f L r ( R N ) .

Lemma 2.3

(Brezis-Lieb lemma [17]) Let s ( 1 , ) and { w n } be a bounded sequence in L s ( R N ) . If w n w almost everywhere on R N , then for any q [ 1 , s ] ,

(7) lim n R N w n q w n w q w q s q d x = 0

and

(8) lim n R N w n q 1 w n w n w q 1 ( w n w ) w q 1 w s q d x = 0 .

Lemma 2.4

(Nonlocal Brezis lemma [6]) Let α ( 0 , N ) , N 3 , p 1 , 2 N N + α and { u n } be a bounded sequence in L 2 N p N + α ( R N ) . If u n u almost everywhere on R N , then

lim n R N ( I α u n p ) u n p d x R N ( I α u n u p ) u n u p d x = R N ( I α u p ) u p d x .

Lemma 2.5

[13] Let α ( 0 , N ) , N 3 , p 1 , 2 N N + α and { u n } be a bounded sequence in L 2 N p N + α ( R N ) . If { u n } u almost everywhere on R N , then for any h L 2 N p N + α ( R N ) ,

lim n R N ( I α u n p ) u n p 2 u n h d x = R N ( I α u p ) u p 2 u h d x .

Lemma 2.6

(Pohozaev identity [6,7,18,19]). Suppose V ( x ) satisfies ( V 1 )–( V 2 ) and let u X be a weak solution of Problem (1), then we have the following Pohozaev identity:

(9) 0 = P V ( u ) = a 2 R 3 u 2 d x + 3 2 R 3 V ( x ) u 2 d x + 1 2 R 3 ( V ( x ) , x ) x 2 d x + b 2 R 3 u 2 d x 2 3 + α 2 p R 3 ( I α u p ) u p d x 3 R 3 F ( u ) d x .

In particular, if V V , we have

(10) 0 = P ( u ) = a 2 R 3 u 2 d x + 3 2 R 3 V u 2 d x + b 2 R 3 u 2 d x 2 3 + α 2 p R 3 ( I α u p ) u p d x 3 R 3 F ( u ) d x .

3 Ground state solution for the “limit problem” of equation (1)

In this section, we will investigate the following limit problem that is associated with problem (1):

(11) ( a + b R 3 u 2 ) Δ u + V u = ( I α u p ) u p 2 u + f ( u ) , in R 3 , u H 1 ( R 3 ) .

The asscoiated energy function is given by:

(12) I ( u ) = 1 2 R 3 [ a u 2 + V u 2 ] d x + b 4 R 3 u 2 d x 2 1 2 p R 3 ( I α u p ) u p d x R 3 F ( u ) d x .

We prove the following results.

Lemma 3.1

Let p 3 + α 3 , 3 + α , then I has no lower bounds.

Proof

For u X \ { 0 } and t > 0 , we have

I ( u t ) = I ( t u ( t 1 x ) ) = a t 2 2 R 3 u 2 d x + t 4 2 R 3 V u 2 d x + b t 4 4 R 3 u 2 d x 2 t p + 3 + α 2 p R 3 ( I α u p ) u p d x t 3 R 3 F ( t u ) d x

as t , since p + 3 + α > 4 , and then we can obtain the conclusion.□

Next we define = { u X \ { 0 } : G ( u ) = 0 } , where

(13) G ( u ) = 1 2 I ( u ) , u + P ( u ) = a R 3 u 2 d x + 2 R 3 V u 2 d x + b R 3 u 2 d x 2 p + 3 + α 2 p R 3 ( I α u p ) u p d x 3 R 3 F ( u ) d x 1 2 R 3 f ( u ) u d x = d I ( u t ) d t t = 1 .

Remark 3.2

For t > 0 , we set

(14) γ ( t ) = I ( u t ) = a t 2 2 R 3 u 2 d x + t 4 2 R 3 V u 2 d x + b t 4 4 R 3 u 2 d x 2 1 2 p t p + 3 + α R 3 ( I α u p ) u p d x t 3 R 3 F ( t u ) d x .

Lemma 3.3

Let c 1 , c 2 , and c 3 be constants, which are positive and u X \ { 0 } . Then, the function

η ( t ) = c 1 t 2 + c 2 t 4 c 3 t ( p + 3 + α ) t 3 R 3 F ( t u ) d x f o r t 0

has only one positive critical point, which corresponds to its maximal value.

Proof

One can obtain the result by elementary calculation.□

Lemma 3.4

For any u X \ { 0 } , there exists only one t 0 > 0 such that u t 0 and I ( u t 0 ) = max t > 0 I ( u t ) .

Proof

I ( u t ) has the form of the function η ( t ) defined earlier. Since by Lemma 3.3, η ( t ) has only one critical point t 0 > 0 , which corresponds to its maximal value. Thus, η ( t 0 ) = max t > 0 η ( t ) and η ( t 0 ) = 0 . It follows that G ( u t 0 ) = t 0 η ( t 0 ) = 0 . This implies u t 0 and I ( u t 0 ) = max t > 0 I ( u t ) .□

Lemma 3.5

The functional I possesses the mountain-pass geometry, i.e.,

  1. there exists ρ , δ > 0 such that I δ for all u = ρ ;

  2. there exists e H 1 ( R 3 ) such that e > ρ and I ( e ) < 0 .

Proof

(1) By Lemmas 2.1(1) and 2.2, we have

I ( u ) c 1 u 2 c 2 u 2 p C ε u q .

Thus, there exists ρ , δ > 0 such that I δ for all u = ρ > 0 small enough.

(2) For any u X \ { 0 } , by the definition of I ( u t ) , we see I ( u t ) < 0 for t > 0 large. Note that

u t 2 = a t 2 R 3 u 2 d x + t 4 R 3 V u 2 d x .

Taking e = u t 0 , with t 0 > 0 large, then we have e > ρ and I ( e ) < 0 .□

Now we can define the mountain-pass level of I :

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

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

Let

m = inf u I ( u ) ,

then for any u , we have

I ( u ) = I ( u ) 1 4 G ( u ) a 4 R 3 u 2 d x 0 .

Thus, m is well defined. In addition, by the similar argument as Chapter 4 [19], we have the following property:

c = inf u X { 0 } max t > 0 I ( u t ) = m = inf u I ( u ) .

Lemma 3.6

Assume that ( f 1)–( f 4) hold, then m is obtained.

Proof

Let { u n } be such that I ( u n ) m . Since G ( u n ) = 0 , we have:

1 + m > I ( u n ) = I ( u n ) 1 4 G ( u n ) = a 4 R 3 u n 2 d x + 1 8 R 3 [ f ( u n ) u n 2 F ( u n ) ] d x + p 1 + α 8 p R 3 ( I α u p ) u p d x > a 4 R 3 u n 2 d x

for n large enough. Therefore, { u n 2 2 } is bounded. So there exists A 0 such that R 3 u n 2 d x A . We claim that { u n 2 2 } is also bounded. By Lemmas 2.1(1) and 2.2(1), the definition of G ( u n ) and Sobolev inequality, we have

2 R 3 V u n 2 d x = 1 2 R 3 [ 6 F ( u n ) d x + f ( u n ) u n ] d x + p + 3 + α 2 p R 3 ( I α u n p ) u n p d x a R 3 u n 2 d x b R 3 u n 2 d x 2 < 1 2 R 3 [ 6 F ( u n ) + f ( u n ) u n ] d x + p + 3 + α 2 p R 3 ( I α u n p ) u n p d x < ε u n 2 2 + C ε u n q q + C u n 6 p 3 + α 2 p < ε u n 2 2 + C ε u n 2 q + C u n 2 2 p ,

which indicates { u n 2 2 } is bounded. Then let δ = lim n sup y R 3 B 1 ( y ) u n 2 d x . Next we prove δ > 0 . If δ = 0 , then by Lions’ concentration compactness principle [19], we have u n 0 in L q ( R 3 ) for q ( 2 , 6 ) . From Lemma 2.2, we can obtain that

R 3 ( I α u n p ) u n p d x C u n 6 p 3 + α 2 p 0 ,

since 2 < 6 p 3 + α < 6 . Together with G ( u n ) = 0 , we have u n 0 in X . This conflicts with the fact that c > 0 . So δ > 0 and there exists { y n } R 3 such that B 1 ( y n ) u n 2 d x δ 2 > 0 . We set v n ( x ) = u n ( x + y n ) , then

u n = v n , B 1 ( 0 ) v n 2 d x > δ 2

and

I ( v n ) m , G ( v n ) = 0 .

Therefore, there exists v X \ { 0 } such that

v n v in X , v n v in L l o c s ( R 3 ) , s [ 1 , 6 ) v n v a . e . on R 3

and R 3 v n 2 d x A . Then, we set

I A , ( u ) = a + b A 2 R 3 u 2 d x + 1 2 R 3 V u 2 d x 1 2 p R 3 ( I α u p ) u p d x R 3 F ( u ) d x .

Since I ( v n ) 0 and v n v in X , we have I A , ( v ) = 0 . Besides v satisfied the following Pohozaev identity:

P A , = a + b A 2 R 3 u 2 d x + 3 2 R 3 V u 2 d x 3 + α 2 p R 3 ( I α u p ) u p d x 3 R 3 F ( u ) d x = 0 .

Suppose that R 3 v 2 d x < A , then we have

0 = I A , ( v ) , v 2 + P A , ( v ) > G ( v ) .

Thus, by Lemma 3.4, there exists t 0 ( 0 , 1 ) such that v t 0 . Hence, we have

c I ( v t 0 ) = I ( v t 0 ) 1 4 G ( v t 0 ) = a t 0 2 4 R 3 v 2 d x + t 0 3 8 R 3 [ f ( t v ) t v 2 F ( t v ) ] d x + p + α 1 8 p t 0 p + 3 + α R 3 ( I α v p ) v p d x < a 4 R 3 v 2 d x + 1 8 R 3 [ f ( v ) v 2 F ( v ) ] d x + p + α 1 8 p R 3 ( I α v p ) v p d x lim n a 4 R 3 v n 2 d x + 1 8 R 3 [ f ( v n ) v n 2 F ( v n ) ] d x + p + α 1 8 p R 3 ( I α v n p ) v n p d x = lim n I ( v n ) 1 4 G ( v n ) = m .

This is a contradiction. Consequently, we obtain R 3 v 2 d x = A = lim n R 3 v n 2 d x . So G ( v ) = 0 , I ( v ) = m . This completes the proof.□

Lemma 3.7

If m is obtained at some u ˜ , then u ˜ is a critical point of I ( u ) .

Proof

It is obvious that u ˜ 0 since u ˜ . Then we claim that for every fixed v H 1 ( R 3 ) , there exists ε > 0 such that u ˜ + s v 0 for all s ( ε , ε ) . In fact, by contradiction, there exists a sequence { s i } i = 1 such that lim i + s i = 0 and u ˜ + s i v = 0 a.e. on R 3 . Letting i + , we have u ˜ = 0 a.e. on R 3 , which is a contradiction with u ˜ 0 . Then by Lemma 3.3, there exists only one t 0 > 0 such that ( u ˜ + s v ) t ( s ) . Now consider the function Φ ( t , s ) = G ( ( u ˜ + s v ) t ) defined for ( t , s ) ( 0 , + ) × ( ε , ε ) . Since u ˜ , one has Φ ( 1 , 0 ) = G ( u ˜ ) = 0 . Moreover, Φ is a C 1 function and

Φ ( t , s ) t ( t , s ) = ( 1 , 0 ) < 0 .

By the implicit function theorem, the function t ( s ) is C 1 and being t ( 0 ) = 1 , then one can know t ( s ) 0 near 0. By letting γ ( s ) = I ( ( u ˜ + s v ) t ( s ) ) , one has γ is differentiable for all small s and attains its minimum at s = 0 . Therefore, we can deduce

0 = γ ( 0 ) = d I ( ( u ˜ + s v ) t ( s ) ) d s s = 0 = I ( ( u ˜ + s v ) t ) t ( t , s ) = ( 1 , 0 ) d t d s t = 0 + I ( ( u ˜ + s v ) t ) s ( t , s ) = ( 1 , 0 ) = G ( u ˜ ) t ( 0 ) + I ( u ˜ ) , v = I ( u ˜ ) , v .

Since v X is arbitrary, we deduce that I ( u ˜ ) = 0 .□

Then by Lemmas 3.6 and 3.7, we can have the following result.

Theorem 3.8

Under assumptions ( f 1 )–( f 4 ), Problem (11) has a ground state solution.

4 Ground state solution for problem (1)

Proposition 4.1

(See [20]) Let ( X , ) be a Banach space and T R + be an interval. Φ τ ( u ) is a family of C 1 functions on X of the following form:

Φ τ ( u ) = A ( u ) τ B ( u ) , τ T ,

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

c τ = inf γ Γ max t [ 0 , 1 ] Φ τ ( γ ( t ) ) > max { Φ τ ( v 1 ) , Φ τ ( v 2 ) } , τ T ,

where Γ = { γ C ( [ 0 , 1 ] , X ) : γ ( 0 ) = v 1 , γ ( 1 ) = v 2 } , then for almost every τ T , there is a bounded ( P S ) c τ sequence in X.

Set T = [ δ , 1 ] , where δ > 0 . We investigate a family of functionals on X with the following form:

I V , τ ( u ) = 1 2 R 3 [ a u 2 + V ( x ) u 2 ] d x + b 4 R 3 u 2 d x 2 τ 1 2 p R 3 ( I α u p ) u p d x + R 3 F ( u ) d x , τ [ δ , 1 ] .

Then we can set I V , τ ( u ) = A ( u ) τ B ( u ) . Here,

A ( u ) = 1 2 R 3 [ a u 2 + V ( x ) u 2 ] d x + b 4 R 3 u 2 d x 2 + ,

as u + , and

B ( u ) = 1 2 p R 3 ( I α u p ) u p d x + R 3 F ( u ) d x 0 .

Lemma 4.2

Assume (V2) holds, then we have

  1. there exists a v X \ { 0 } such that I V , τ ( v ) 0 for all τ [ δ , 1 ] ,

  2. c τ = inf γ Γ max t [ 0 , 1 ] I V , τ ( γ ( t ) ) > max { I V , τ ( 0 ) , I V , τ ( v ) } for all τ [ δ , 1 ] , where

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

Proof

(1) Fix u X \ { 0 } , then for τ [ δ , 1 ] and t > 0 , we have

I V , τ ( u t ) I V , δ ( u t ) = a t 2 2 R 3 u 2 d x + t 4 2 R 3 V u 2 d x + b t 4 4 R 3 u 2 d x 2 δ t p + 3 + α 2 p R 3 ( I α u p ) u p d x + t 3 R 3 F ( t u ) d x

as t + . Just by taking v = u t with t large, one can have

I V , τ ( u t ) I V , δ ( u t ) < 0 .

(2) By Lemmas 2.1(1) and 2.2, we have

I V , τ ( u ) c 1 u 2 c 2 u 2 p C ε u q .

Since p > 1 , I V , τ ( u ) has a strictly local minima at 0, i.e., there exists r > 0 such that

b = inf u = r I V , τ ( u ) > 0 = I V , τ ( 0 ) I V , τ ( v ) ,

and hence taking u t = v , we obtain c τ > max { I V , τ ( 0 ) , I V , τ ( u t ) } = 0 .□

Lemma 4.3

(See [20]) Assume the conditions of Proposition 4.1 hold, the map τ c τ is nonincreasing and left continuous.

By Theorem 3.8, we conclude that for τ [ δ , 1 ] , the “limit problem” of the following type

(15) ( a + b R 3 u 2 ) Δ u + V u = τ [ ( I α u p ) u p 2 u + f ( u ) ] , in R 3 , u H 1 ( R 3 )

has a ground state solution u τ H 1 ( R 3 ) , i.e., for τ [ δ , 1 ] , there exists u τ τ = { u X \ { 0 } : G , τ ( u ) = 0 } such that I V , τ ( u τ ) = 0 and I V , τ ( u τ ) = m τ = inf u τ I V , τ ( u ) . Here,

I V , τ ( u ) = 1 2 R 3 [ a u 2 + V u 2 ] d x + b 4 R 3 u 2 d x 2 τ 1 2 p R 3 ( I α u p ) u p d x + R 3 F ( u ) d x ,

G , τ ( u ) = a R 3 u 2 d x + 2 R 3 V u 2 d x + b R 3 u 2 d x 2 p + 3 + α 2 p τ R 3 ( I α u p ) u p d x 3 τ R 3 F ( u ) d x τ 2 R 3 f ( u ) u d x .

Lemma 4.4

Suppose that ( V 1 )–( V 2 ) hold, and V ( x ) V , then c τ < m τ for τ [ δ , 1 ] .

Proof

Let u τ be the minimizer of m τ . By Lemma 4.2, there exists t ˜ ( 0 , t 0 ) such that

c τ = inf γ Γ max t [ 0 , 1 ] I V , τ ( γ ( t ) ) max 0 < t < t 0 I V , τ t u τ x t = I V , τ t ˜ u τ x t ˜ < I V , τ t ˜ u τ x t ˜ max t > 0 I V , τ t u τ x t = I V , τ ( u τ ) = m τ .

Next we provide the following global compactness lemma.

Lemma 4.5

(See [3,13]) Suppose that ( V 1 )–( V 2 ) and ( f 1 )–( f 4 ) hold. For c > 0 and τ [ δ , 1 ] , let { u n } X be a bounded ( P S ) c sequence for I V , τ . Then there exists a u 0 X and A R such that J V , τ ( u 0 ) = 0 . Here,

J V , τ ( u ) = a + b A 2 2 R 3 a u 2 d x + 1 2 R 3 V ( x ) u 2 d x τ 1 2 p R 3 ( I α u p ) u p d x + R 3 F ( u ) d x .

Moreover, either

  1. u n u 0 strongly in H 1 ( R 3 ) , or

  2. there exists a finite(possibly empty) set u 1 , u 2 , , u k X of nontrivial solutions of

    ( a + b A 2 ) Δ u + V u = τ [ ( I α u p ) u p 2 u + f ( u ) ] ,

    and y n i R 3 , i = 1 , 2 , 3 , , k ( k N + ) , such that

    y n i , y n i y n j ( i i ) , a s n ;

    c + b A 4 4 = J V , τ ( u 0 ) + i = 1 k J V , τ ( u i ) ;

    u n u 0 i = 1 k ( y n i ) u i 0 ;

    A 2 = u 0 2 2 + i = 1 k u i 2 2 ,

where

J V , τ ( u ) = a + b A 2 2 R 3 a u 2 d x + 1 2 R 3 V u 2 d x τ 1 2 p R 3 ( I α u p ) u p d x + R 3 F ( u ) d x .

Lemma 4.6

(See [3,13]) Suppose that ( V 1 )–( V 2 ) and ( f 1 )–( f 4 ) hold. For τ [ δ , 1 ] , let { u n } X be a bounded ( P S ) c τ sequence for I V , τ . Then there exists a nontrivial u τ X such that u n u τ strongly in X.

Now, we can prove the main theorem.

Proof of Theorem 1.1

In the view of Proposition 4.1 and Lemma 4.2, we see for a.e. τ [ δ , 1 ] , there exists a bounded sequence { u n } X such that I V , τ ( u n ) c τ , I V , τ ( u n ) 0 . By Lemma 4.6, I V , τ has a nontrivial critical point u τ X and I V , τ ( u τ ) = c τ for a.e. τ [ δ , 1 ] . Next, we choose an arbitrary sequence { τ n } [ δ , 1 ] with τ n 1 , then we obtain a sequence { u τ n } X such that I V , τ n ( u τ n ) = 0 and I V , τ n ( u τ n ) = c τ n . In the following, we show that { u τ n } is bounded in X . By ( V 1 ) and Hardy inequality, using the similar argument in Lemma 3.5, we can derive that both u τ n 2 and u τ n 2 are bounded. Thus, { u τ n } is bounded in X .

On the other hand, since τ n 1 , by Lemma 4.3, we have

lim n I ( u τ n ) = lim n I V , 1 ( u τ n ) = lim n I V , τ n ( u τ n ) + ( τ n 1 ) 1 2 p R 3 ( I α u τ n p ) u τ n p d x + R 3 F ( u τ n ) d x = lim n c τ n = c 1

and

lim n I ( u τ n ) , φ = lim n I V , 1 ( u τ n ) , φ = lim n I V , τ n ( u τ n ) , φ + ( τ n 1 ) R 3 ( I α u τ n p ) u τ n p 2 u τ n φ d x + R 3 f ( u τ n ) φ d x = 0 .

That is { u τ n } is a bounded ( P S ) c 1 sequence for I . Again by Lemma 4.6, there exists u 0 X such that I ( u 0 ) = c 1 , I ( u 0 ) = 0 , which means u 0 is a nontrivial solution of Problem (1).

Finally, we prove the existence of ground state solution. Set m = inf S I ( u ) , where S = { u X \ { 0 } : I ( u ) = 0 } . Now we show 0 < m < . Since u 0 S , we see m c 1 < . For any u S , we have

0 = I ( u ) , u = a R 3 u 2 d x + R 3 V ( x ) u 2 d x + b R 3 u 2 d x 2 R 3 ( I α u p ) u p d x R 3 f ( u ) u d x c 1 u 2 c 2 u 2 p C ε u q .

This indicates that u δ for some δ > 0 . On the other hand, by the Pohozaev identity, i.e., P V ( u ) = 0 . Then by ( V 1 ) and Hardy’s inequality, we obtain:

I ( u ) = I ( u ) 1 8 [ I ( u ) , u + 2 P V ( u ) ] = a 4 R 3 u 2 d x 1 8 R 3 ( V ( x ) , x ) u 2 d x + p + α 1 8 p R 3 ( I α u p ) u p d x + 1 8 R 3 [ u f ( u ) 2 F ( u ) ] d x a 4 R 3 u 2 d x 1 8 R 3 ( V ( x ) , x ) u 2 d x a 4 R 3 u 2 d x A 16 R 3 u 2 x 2 d x a 4 R 3 u 2 d x A 4 R 3 u 2 d x = a A 4 R 3 u 2 d x .

This implies m 0 . In the following, let us rule out m = 0 . If m = 0 , then there exists minimizing sequence { u n } S such that I ( u n ) 0 , which implies lim n R 3 u n 2 d x = 0 . Since I ( u n ) , u n = 0 , we can infer lim n R 3 u n 2 d x = 0 . Therefore, lim n u n 2 = 0 , which contradicts to u n > δ . This proves our claim.

Then let { u n } S be a minimizing sequence such that I ( u n ) = 0 and I ( u n ) m . By similar argument as mentioned earlier, one can conclude that { u n } is bounded. Again by Lemma 4.6, there exists a u X such that u n u strongly in X . Thus, I ( u ) = 0 , I ( u ) = m . This implies u is a ground state solution for Problem (1). Then we finish the proof.□

5 Ground state solution for problem (2)

As we all know, a weak solution of Problem (2) is a critical point of the following functional:

J m ( u ) = 1 2 R 3 [ a u 2 + V ( x ) u 2 ] d x + b 4 R 3 u 2 d x 2 1 2 p R 3 ( I α u p ) u p d x m l R 3 u l d x .

But obviously we cannot apply variational methods directly because that the functional J m is not well defined when l > 6 . To solve this difficulty, we define the following function:

φ ( t ) = t l 2 t if t M , M l q t q 2 t if t > M .

where M > 0 . Then φ C ( R , R ) and φ ( t ) M l q t q 1 for all t R . Thus, m φ ( t ) ( m > 0 ) verifies the conditions ( f 1 )–( f 4 ). By Theorem 1.1, we know the equation:

(16) a + b R 3 u 2 Δ u + V ( x ) u = ( I α u p ) u p 2 u + m φ ( t ) , in R 3

has a ground state solution u m .

Let

J ˜ m ( u ) = 1 2 R 3 [ a u 2 + V ( x ) u 2 ] d x + b 4 R 3 u 2 d x 2 1 2 p R 3 ( I α u p ) u p d x m R 3 Φ ( u ) d x ,

where Φ ( t ) = 0 t φ ( s ) d s . As a consequence, J ˜ m ( u m ) = c m , and J ˜ m ( u m ) = 0 . By characterization of minimax level, we can derive that

c m = inf γ Γ m max t [ 0 , 1 ] J ˜ m ( γ ( t ) ) ,

where

Γ m = { γ C ( [ 0 , 1 ] , X ) : γ ( 0 ) = 0 , J ˜ m ( γ ( 1 ) ) < 0 } .

Next, set

J ( u ) = 1 2 R 3 [ a u 2 + V ( x ) u 2 ] d x + b 4 R 3 u 2 d x 2 1 2 p R 3 ( I α u p ) u p d x R 3 Φ ( u ) d x ,

and

c = inf γ Γ max t [ 0 , 1 ] J ( γ ( t ) ) ,

where

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

Then obviously we have Γ Γ m and c m c .

Next we only need to prove the following lemmas.

Lemma 5.1

The solution u m satisfies u m 2 2 4 c m a A , and there exists a constant A > 0 , which is independent on m such that u m 2 2 A

Proof

By Pohozaev identity, ( V 1 ) and Hardy inequality, we have

c m = J ˜ m ( u m ) 1 8 [ J ˜ m ( u m ) , u m + 2 P V ( u m ) ] = a 4 R 3 u m 2 d x 1 8 R 3 ( V ( x ) , x ) u m 2 d x + p + α 1 8 p R 3 ( I α u m p ) u m p d x + m 8 R 3 [ u m φ ( u m ) 2 Φ ( u m ) ] d x a 4 R 3 u m 2 d x 1 8 R 3 ( V ( x ) , x ) u m 2 d x a 4 R 3 u m 2 d x A 16 R 3 u m 2 x 2 d x a 4 R 3 u m 2 d x A 4 R 3 u m 2 d x = a A 4 R 3 u m 2 d x ,

which implies u m 2 2 4 c m a A 4 c a A A > 0 . This completes the proof.□

By some parts of the ideas of the proof, which comes from [14,15], we can obtain the following lemma.

Lemma 5.2

There exist two constants B , D > 0 , which is independent on m such that u m L B ( 1 + m ) D .

Proof

Set I > 2 , r > 0 and u ˜ m I b ( u m ) , where b : R R is a smooth function, which satisfies b ( s ) = s for s I 1 , b ( s ) = b ( s ) ; b ( s ) = 0 for s I and b ( s ) is decreasing in [ I 1 , I ] . This implies that

u ˜ m I = u m , for u m I 1 , u ˜ m I = b ( u m ) u m , for I 1 u m I , u ˜ m I = C I > 0 , for u m I ,

where I 1 C I I . Moreover, one can easily have

0 s b ( s ) b ( s ) 1 , s 0 .

Let ψ = u m u ˜ m I 2 r . Then ψ X , if one takes ψ as the test function, one can have

(17) R 3 ( I α u m p ) u m p 2 u m ψ d x + m R 3 φ ( u m ) ψ = a R 3 u m ψ d x + b R 3 u m 2 d x R 3 u m ψ d x + R 3 V ( x ) u m ψ d x .

Note that

R 3 u m ψ d x u m I 1 ( 1 + r ) u ˜ m I 2 r u m 2 d x + u m I u ˜ m I 2 r u m 2 d x + I 1 < u m < I [ u ˜ m I 2 r + 2 r u m b ( u m ) b ( u m ) u ˜ m I 2 r 2 ] u m 2 d x u m I 1 u ˜ m I 2 r u m 2 d x + u m I u ˜ m I 2 r u m 2 d x + I 1 < u m < I [ u ˜ m I 2 r + 2 r u m b ( u m ) b ( u m ) u ˜ m I 2 r 2 ] u m 2 d x 1 ( 1 + r ) 2 u m I 1 [ u m ( u ˜ m I ) r ] 2 d x + u m I [ u m ( u ˜ m I ) r ] 2 d x + I 1 < u m < I [ u ˜ m I 2 r + 2 r u m 2 ( b ( u m ) ) 2 u ˜ m I 2 r 2 ] u m 2 d x 1 ( 1 + r ) 2 u m I 1 [ u m ( u ˜ m I ) r ] 2 d x + u m I [ u m ( u ˜ m I ) r ] 2 d x + I 1 < u m < I 1 ( 1 + r ) 2 u ˜ m I 2 r + r ( 1 + r ) 2 2 r u m 2 ( b ( u m ) ) 2 u ˜ m I 2 r 2 u m 2 d x = 1 ( 1 + r ) 2 u m I 1 [ u m ( u ˜ m I ) r ] 2 d x + u m I [ u m ( u ˜ m I ) r ] 2 d x + I 1 < u m < I 1 ( 1 + r ) 2 b 2 r ( u m ) u m 2 + 2 ( 1 + r ) 2 u m 2 b r ( u m ) 2 d x 1 ( 1 + r ) 2 u m I 1 [ u m ( u ˜ m I ) r ] 2 d x + u m I [ u m ( u ˜ m I ) r ] 2 d x + 2 C 1 ( 1 + r ) 2 I 1 < u m < I [ b 2 r ( u m ) u m 2 + u m 2 b r ( u m ) 2 ] d x 1 ( 1 + r ) 2 u m I 1 [ u m ( u ˜ m I ) r ] 2 d x + u m I [ u m ( u ˜ m I ) r ] 2 d x + C 1 ( 1 + r ) 2 I 1 < u m < I [ u m ( u ˜ m I ) r ] 2 d x C 1 ( 1 + r ) 2 R 3 [ u m ( u ˜ m I ) r ] 2 d x .

Hence, by (17), we obtain

R 3 ( I α u m p ) u m p u ˜ m I 2 r d x + m R 3 φ ( u m ) u m u ˜ m I 2 r d x C 1 ( 1 + r ) 2 R 3 [ u m ( u ˜ m I ) r ] 2 d x + R 3 V ( x ) u m 2 u ˜ m I 2 r d x .

For any ε > 0 , by Lemma 5.1, properties of u ˜ m I and φ , there exists C ε > 0 such that

R 3 ( I α u m p ) u m p u ˜ m I 2 r d x I 1 R 3 ( I α u m p ) u m p d x I 2 u m 6 p 3 + α 2 p < C u m 2 2 p M ,

where I 1 , I 2 , and M are positive constants, and

φ ( t ) ε t + C ε t 2 1

for all t R , where 2 = 2 N N 2 if N 3 and 2 = if N = 1 or 2. Thus, for fixed m > 0 and small ε > 0 , we have

C 1 ( 1 + r ) 2 R 3 [ u m ( u ˜ m I ) r ] 2 d x R 3 ( I α u m p ) u m p u ˜ m I 2 r d x + m R 3 φ ( u m ) u m u ˜ m I 2 r d x R 3 V ( x ) u m 2 u ˜ m I 2 r d x M + R 3 V 0 u m 2 u ˜ m I 2 r d x + m C R 3 u m 2 u ˜ m I 2 r d x R 3 V 0 u m 2 u ˜ m I 2 r d x ( 1 + m ) C R 3 u m 2 u ˜ m I 2 r d x .

Notice that

C 2 ( 1 + r ) 2 R 3 u m 2 u ˜ m I 2 r 2 2 d x 2 2 C 1 ( 1 + r ) 2 R 3 [ u m ( u ˜ m I ) r ] 2 d x .

Consequently,

R 3 u m 2 u ˜ m I 2 r 2 2 d x 2 2 ( 1 + m ) C ( r + 1 ) 2 R 3 u m 2 u ˜ m I 2 r d x .

Take r 0 > 0 and r k = r 0 2 2 k = r k 1 2 2 . Then

(18) R 3 u m 2 u ˜ m I 2 r k d x 1 2 r k [ 1 + m C ( r k 1 + 1 ) ] 1 r k 1 R 3 u m 2 u ˜ m I 2 r k 1 d x 1 2 r k 1 i = 0 k 1 [ 1 + m C ( r i + 1 ) ] 1 r i R 3 u m 2 u ˜ m I 2 r 0 d x 1 2 r 0 = i = 0 k 1 ( 1 + m ) 1 2 r i i = 0 k 1 [ C ( r i + 1 ) ] 1 r i R 3 u m 2 u ˜ m I 2 r 0 d x 1 2 r 0 = i = 0 k 1 ( 1 + m ) 1 2 r i exp i = 0 k 1 1 r i ln [ C ( r i + 1 ) ] R 3 u m 2 u ˜ m I 2 r 0 d x 1 2 r 0 .

Notice that

R 3 u m 2 u ˜ m I 2 r 0 N N 2 d x N 2 N C ( r 0 + 1 ) 2 R 3 u m 2 u ˜ m I 2 r 0 d x C ( r 0 + 1 ) 2 u m ( x ) < ρ u m 2 u ˜ m I 2 r 0 d x + C ( r 0 + 1 ) 2 u m ( x ) ρ u m 2 d x 2 N R 3 u m 2 u ˜ m I 2 r 0 N N 2 d x N 2 N .

Take ρ > 0 be such that

C ( r 0 + 1 ) 2 u m ( x ) ρ u m 2 d x 2 N < 1 2 .

Then

R 3 u m 2 u ˜ m I 2 r 0 N N 2 d x N 2 N C ( r 0 + 1 ) 2 u m ( x ) < ρ u m 2 u ˜ m I 2 r 0 d x C .

Set

d k = i = 0 k 1 [ C ( r i + 1 ) ] 1 r i = exp i = 0 k 1 1 r i ln [ C ( r i + 1 ) ]

and

e k = i = 0 k 1 ( 1 + m ) 1 2 r i = ( 1 + m ) 2 ( 2 2 ) 2 r 0 1 2 2 k .

Then d k d as k and e k e = ( 1 + m ) 2 ( 2 2 ) 2 r 0 as k . By (18) and Lemma 5.1, we have

(19) R 3 u m 2 u ˜ m I 2 r k d x 1 2 r k d k e k R 3 u m 2 u ˜ m I 2 r 0 d x 1 2 r 0 d k e k R 3 u m 2 d x 2 N R 3 u m 2 u ˜ m I 2 r 0 N N 2 d x N 2 N 1 2 r 0 C d k e k R 3 u m 2 d x 1 N r 0 C d k e k .

From (19), by Fatou Lemma with T + , one has

u m 2 + 2 r k 2 + 2 r k 2 r k C d k e k .

Consequence, let k , we obtain

u m L C d e = C d ( 1 + m ) 2 ( 2 2 ) 2 r 0 B ( 1 + m ) D ,

where B > 0 and D > 0 . Now we complete the proof.□

Proof of Theorem 1.2

By Lemma 5.2, for large M > 0 , we can choose small m 0 > 0 such that u m L B ( 1 + m ) D M for all m ( 0 , m 0 ] . Consequently, u m is a ground state solution of equation (2) with m ( 0 , m 0 ] . Finally, we finish the proof.□

  1. Funding information: Our work was supported by National Natural Science Foundation of China (Grant Nos. 11771198 and 11901276) and Science and Technology project of Education Department of Jiangxi Province (Grant No. GJJ218406).

  2. Author contributions: Conceptualization, Li Zhou and Chuanxi Zhu; methodology, Li Zhou; software, Li Zhou; validation, Li Zhou; formal analysis, Li Zhou; investigation, Li Zhou; resources, Chuanxi Zhu; data curation, Li Zhou; writing–original draft preparation, Li Zhou; writing–review and editing, Li Zhou and Chuanxi Zhu; supervision, Chuanxi Zhu; project administration, Chuanxi Zhu; funding acquisition, Chuanxi Zhu. All authors have read and agreed to the published version of the manuscript.

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

  4. Data availability statement: Not applicable. No data, models, or code were generated or used during the study.

References

[1] Y. Li, Z. Q. Wang, and J. Zeng, Ground states of nonlinear Schrödinger equations with potentials, Ann. Inst. H. Poincaré C Anal. Non Linéare 23 (2006), 829–837. 10.1016/j.anihpc.2006.01.003Search in Google Scholar

[2] Z. Liu and Z. Q. Wang, On the Ambrosetti-Rabinowitz superlinear condition, Adv. Nonlinear Stud. 4 (2004), 561–572. 10.1515/ans-2004-0411Search in Google Scholar

[3] Z. Guo, Ground states for Kirchhoff equations without compact condition, J. Differential Equations 259 (2015), 2884–2902. 10.1016/j.jde.2015.04.005Search in Google Scholar

[4] D. Ruiz, The Schrdinger-Poisson equation under the effect of a nonlinear local term, J. Funct. Anal. 237 (2006), no. 2, 655–674. 10.1016/j.jfa.2006.04.005Search in Google Scholar

[5] I. M. Moroz, R. Penrose, and P. Tod, Spherically-symmetric solutions of Schrödinger-Newton equations, Classical Quantum Gravity 15 (1998), 2733–2742. 10.1088/0264-9381/15/9/019Search in Google Scholar

[6] V. Moroz and J. Van Schaftingen, Ground states of nonlinear Choquard equations: existence, qualitative properties and decay asymptotics, J. Funct. Anal. 265 (2013), 153–184. 10.1016/j.jfa.2013.04.007Search in Google Scholar

[7] V. Moroz and J. Van Schaftingen, Existence of ground states for a class of nonlinear Choquard equations, Trans. Amer. Math. Soc. 367 (2015), 6557–6579. 10.1090/S0002-9947-2014-06289-2Search in Google Scholar

[8] V. Moroz and J. Van Schaftingen, Nonexistence and optimal decay of supersolutions to Choquard equations in exterior domains, J. Differential Equations 254 (2013), 3089–3145. 10.1016/j.jde.2012.12.019Search in Google Scholar

[9] V. Moroz and J. Van Schaftingen, Ground states of nonlinear Choquard equations: Hardy-Littlewood-Sobolev critical exponent, Commun. Contemp. Math. 17 (2015), 1550005. 10.1142/S0219199715500054Search in Google Scholar

[10] V. Moroz and J. Van Schaftingen, A guide to the Choquard equation, J. Fixed Point Theory Appl. 19 (2017), 773–813. 10.1007/s11784-016-0373-1Search in Google Scholar

[11] M. Chimenti and J. Van Schaftingen, Nodal solutions for the Choquard equation, J. Funct. Anal. 271 (2016), 107–135. 10.1016/j.jfa.2016.04.019Search in Google Scholar

[12] L. Ma and Z. Lin, Classification of positive solitary solutions of the nonlinear Choquard equation, Arch. Ration. Mech. Anal. 195 (2010), 455–467. 10.1007/s00205-008-0208-3Search in Google Scholar

[13] P. Chen and X. C. Liu, Ground states for Kirchhoff equation with Hartree-type nonlinearities, J. Math. Anal. Appl. 473 (2019), 587–608. 10.1016/j.jmaa.2018.12.076Search in Google Scholar

[14] Q. Li, K. M. Teng, and X. Wu, Ground states for Kirchhoff-type equations with critical or supercritical growth, Math. Methods Appl. Sci. 40 (2017), 6732–6746. 10.1002/mma.4485Search in Google Scholar

[15] Q. Li, K. M. Teng, and X. Wu, Existence of nontrivial solutions for Schrödinger-Kirchhoff-type equations with critical or supercritical growth, Math. Methods Appl. Sci. 41 (2018), 1136–1144. 10.1002/mma.4652Search in Google Scholar

[16] E. H. Lieb and M. Loss, Analysis, 2nd ed, Grad. Stud. Math, vol. 14, American Mathematical Society, Province, RL, 2001. 10.1090/gsm/014Search in Google Scholar

[17] H. Brézis and E. H. Lieb, A relation between pointwise convergence of functions and convergence of functionals, Proc. Amer. Math. Soc. 88 (1983), 486–490. 10.1007/978-3-642-55925-9_42Search in Google Scholar

[18] H. Berestycki and P. L. Lions, Nonlinear scalar field equations I, Arch. Ration. Mech. Anal. 82 (1983), 313–346. 10.1007/BF00250555Search in Google Scholar

[19] M. Willem, Minimax theorems, Progress in Nonlinear Differential Equations and Their Applications, vol. 24, Birkhäuser, Boston, MA, 1996. 10.1007/978-1-4612-4146-1Search in Google Scholar

[20] L. Jeanjean, On the existence of bounded Palais-Snale sequences and application to a Landsman-Lazer-type problem set on RN, Proc. Edinb. Math. Soc. 129 (1999), no. 2, 787–809. 10.1017/S0308210500013147Search in Google Scholar

Received: 2021-12-05
Revised: 2022-04-01
Accepted: 2022-05-16
Published Online: 2022-08-29

© 2022 Li Zhou and Chuanxi Zhu, published by De Gruyter

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

Articles in the same Issue

  1. Regular Articles
  2. A random von Neumann theorem for uniformly distributed sequences of partitions
  3. Note on structural properties of graphs
  4. Mean-field formulation for mean-variance asset-liability management with cash flow under an uncertain exit time
  5. The family of random attractors for nonautonomous stochastic higher-order Kirchhoff equations with variable coefficients
  6. The intersection graph of graded submodules of a graded module
  7. Isoperimetric and Brunn-Minkowski inequalities for the (p, q)-mixed geominimal surface areas
  8. On second-order fuzzy discrete population model
  9. On certain functional equation in prime rings
  10. General complex Lp projection bodies and complex Lp mixed projection bodies
  11. Some results on the total proper k-connection number
  12. The stability with general decay rate of hybrid stochastic fractional differential equations driven by Lévy noise with impulsive effects
  13. Well posedness of magnetohydrodynamic equations in 3D mixed-norm Lebesgue space
  14. Strong convergence of a self-adaptive inertial Tseng's extragradient method for pseudomonotone variational inequalities and fixed point problems
  15. Generic uniqueness of saddle point for two-person zero-sum differential games
  16. Relational representations of algebraic lattices and their applications
  17. Explicit construction of mock modular forms from weakly holomorphic Hecke eigenforms
  18. The equivalent condition of G-asymptotic tracking property and G-Lipschitz tracking property
  19. Arithmetic convolution sums derived from eta quotients related to divisors of 6
  20. Dynamical behaviors of a k-order fuzzy difference equation
  21. The transfer ideal under the action of orthogonal group in modular case
  22. The multinomial convolution sum of a generalized divisor function
  23. Extensions of Gronwall-Bellman type integral inequalities with two independent variables
  24. Unicity of meromorphic functions concerning differences and small functions
  25. Solutions to problems about potentially Ks,t-bigraphic pair
  26. Monotonicity of solutions for fractional p-equations with a gradient term
  27. Data smoothing with applications to edge detection
  28. An ℋ-tensor-based criteria for testing the positive definiteness of multivariate homogeneous forms
  29. Characterizations of *-antiderivable mappings on operator algebras
  30. Initial-boundary value problem of fifth-order Korteweg-de Vries equation posed on half line with nonlinear boundary values
  31. On a more accurate half-discrete Hilbert-type inequality involving hyperbolic functions
  32. On split twisted inner derivation triple systems with no restrictions on their 0-root spaces
  33. Geometry of conformal η-Ricci solitons and conformal η-Ricci almost solitons on paracontact geometry
  34. Bifurcation and chaos in a discrete predator-prey system of Leslie type with Michaelis-Menten prey harvesting
  35. A posteriori error estimates of characteristic mixed finite elements for convection-diffusion control problems
  36. Dynamical analysis of a Lotka Volterra commensalism model with additive Allee effect
  37. An efficient finite element method based on dimension reduction scheme for a fourth-order Steklov eigenvalue problem
  38. Connectivity with respect to α-discrete closure operators
  39. Khasminskii-type theorem for a class of stochastic functional differential equations
  40. On some new Hermite-Hadamard and Ostrowski type inequalities for s-convex functions in (p, q)-calculus with applications
  41. New properties for the Ramanujan R-function
  42. Shooting method in the application of boundary value problems for differential equations with sign-changing weight function
  43. Ground state solution for some new Kirchhoff-type equations with Hartree-type nonlinearities and critical or supercritical growth
  44. Existence and uniqueness of solutions for the stochastic Volterra-Levin equation with variable delays
  45. Ambrosetti-Prodi-type results for a class of difference equations with nonlinearities indefinite in sign
  46. Research of cooperation strategy of government-enterprise digital transformation based on differential game
  47. Malmquist-type theorems on some complex differential-difference equations
  48. Disjoint diskcyclicity of weighted shifts
  49. Construction of special soliton solutions to the stochastic Riccati equation
  50. Remarks on the generalized interpolative contractions and some fixed-point theorems with application
  51. Analysis of a deteriorating system with delayed repair and unreliable repair equipment
  52. On the critical fractional Schrödinger-Kirchhoff-Poisson equations with electromagnetic fields
  53. The exact solutions of generalized Davey-Stewartson equations with arbitrary power nonlinearities using the dynamical system and the first integral methods
  54. Regularity of models associated with Markov jump processes
  55. Multiplicity solutions for a class of p-Laplacian fractional differential equations via variational methods
  56. Minimal period problem for second-order Hamiltonian systems with asymptotically linear nonlinearities
  57. Convergence rate of the modified Levenberg-Marquardt method under Hölderian local error bound
  58. Non-binary quantum codes from constacyclic codes over 𝔽q[u1, u2,…,uk]/⟨ui3 = ui, uiuj = ujui
  59. On the general position number of two classes of graphs
  60. A posteriori regularization method for the two-dimensional inverse heat conduction problem
  61. Orbital stability and Zhukovskiǐ quasi-stability in impulsive dynamical systems
  62. Approximations related to the complete p-elliptic integrals
  63. A note on commutators of strongly singular Calderón-Zygmund operators
  64. Generalized Munn rings
  65. Double domination in maximal outerplanar graphs
  66. Existence and uniqueness of solutions to the norm minimum problem on digraphs
  67. On the p-integrable trajectories of the nonlinear control system described by the Urysohn-type integral equation
  68. Robust estimation for varying coefficient partially functional linear regression models based on exponential squared loss function
  69. Hessian equations of Krylov type on compact Hermitian manifolds
  70. Class fields generated by coordinates of elliptic curves
  71. The lattice of (2, 1)-congruences on a left restriction semigroup
  72. A numerical solution of problem for essentially loaded differential equations with an integro-multipoint condition
  73. On stochastic accelerated gradient with convergence rate
  74. Displacement structure of the DMP inverse
  75. Dependence of eigenvalues of Sturm-Liouville problems on time scales with eigenparameter-dependent boundary conditions
  76. Existence of positive solutions of discrete third-order three-point BVP with sign-changing Green's function
  77. Some new fixed point theorems for nonexpansive-type mappings in geodesic spaces
  78. Generalized 4-connectivity of hierarchical star networks
  79. Spectra and reticulation of semihoops
  80. Stein-Weiss inequality for local mixed radial-angular Morrey spaces
  81. Eigenvalues of transition weight matrix for a family of weighted networks
  82. A modified Tikhonov regularization for unknown source in space fractional diffusion equation
  83. Modular forms of half-integral weight on Γ0(4) with few nonvanishing coefficients modulo
  84. Some estimates for commutators of bilinear pseudo-differential operators
  85. Extension of isometries in real Hilbert spaces
  86. Existence of positive periodic solutions for first-order nonlinear differential equations with multiple time-varying delays
  87. B-Fredholm elements in primitive C*-algebras
  88. Unique solvability for an inverse problem of a nonlinear parabolic PDE with nonlocal integral overdetermination condition
  89. An algebraic semigroup method for discovering maximal frequent itemsets
  90. Class-preserving Coleman automorphisms of some classes of finite groups
  91. Exponential stability of traveling waves for a nonlocal dispersal SIR model with delay
  92. Existence and multiplicity of solutions for second-order Dirichlet problems with nonlinear impulses
  93. The transitivity of primary conjugacy in regular ω-semigroups
  94. Stability estimation of some Markov controlled processes
  95. On nonnil-coherent modules and nonnil-Noetherian modules
  96. N-Tuples of weighted noncommutative Orlicz space and some geometrical properties
  97. The dimension-free estimate for the truncated maximal operator
  98. A human error risk priority number calculation methodology using fuzzy and TOPSIS grey
  99. Compact mappings and s-mappings at subsets
  100. The structural properties of the Gompertz-two-parameter-Lindley distribution and associated inference
  101. A monotone iteration for a nonlinear Euler-Bernoulli beam equation with indefinite weight and Neumann boundary conditions
  102. Delta waves of the isentropic relativistic Euler system coupled with an advection equation for Chaplygin gas
  103. Multiplicity and minimality of periodic solutions to fourth-order super-quadratic difference systems
  104. On the reciprocal sum of the fourth power of Fibonacci numbers
  105. Averaging principle for two-time-scale stochastic differential equations with correlated noise
  106. Phragmén-Lindelöf alternative results and structural stability for Brinkman fluid in porous media in a semi-infinite cylinder
  107. Study on r-truncated degenerate Stirling numbers of the second kind
  108. On 7-valent symmetric graphs of order 2pq and 11-valent symmetric graphs of order 4pq
  109. Some new characterizations of finite p-nilpotent groups
  110. A Billingsley type theorem for Bowen topological entropy of nonautonomous dynamical systems
  111. F4 and PSp (8, ℂ)-Higgs pairs understood as fixed points of the moduli space of E6-Higgs bundles over a compact Riemann surface
  112. On modules related to McCoy modules
  113. On generalized extragradient implicit method for systems of variational inequalities with constraints of variational inclusion and fixed point problems
  114. Solvability for a nonlocal dispersal model governed by time and space integrals
  115. Finite groups whose maximal subgroups of even order are MSN-groups
  116. Symmetric results of a Hénon-type elliptic system with coupled linear part
  117. On the connection between Sp-almost periodic functions defined on time scales and ℝ
  118. On a class of Harada rings
  119. On regular subgroup functors of finite groups
  120. Fast iterative solutions of Riccati and Lyapunov equations
  121. Weak measure expansivity of C2 dynamics
  122. Admissible congruences on type B semigroups
  123. Generalized fractional Hermite-Hadamard type inclusions for co-ordinated convex interval-valued functions
  124. Inverse eigenvalue problems for rank one perturbations of the Sturm-Liouville operator
  125. Data transmission mechanism of vehicle networking based on fuzzy comprehensive evaluation
  126. Dual uniformities in function spaces over uniform continuity
  127. Review Article
  128. On Hahn-Banach theorem and some of its applications
  129. Rapid Communication
  130. Discussion of foundation of mathematics and quantum theory
  131. Special Issue on Boundary Value Problems and their Applications on Biosciences and Engineering (Part II)
  132. A study of minimax shrinkage estimators dominating the James-Stein estimator under the balanced loss function
  133. Representations by degenerate Daehee polynomials
  134. Multilevel MC method for weak approximation of stochastic differential equation with the exact coupling scheme
  135. Multiple periodic solutions for discrete boundary value problem involving the mean curvature operator
  136. Special Issue on Evolution Equations, Theory and Applications (Part II)
  137. Coupled measure of noncompactness and functional integral equations
  138. Existence results for neutral evolution equations with nonlocal conditions and delay via fractional operator
  139. Global weak solution of 3D-NSE with exponential damping
  140. Special Issue on Fractional Problems with Variable-Order or Variable Exponents (Part I)
  141. Ground state solutions of nonlinear Schrödinger equations involving the fractional p-Laplacian and potential wells
  142. A class of p1(x, ⋅) & p2(x, ⋅)-fractional Kirchhoff-type problem with variable s(x, ⋅)-order and without the Ambrosetti-Rabinowitz condition in ℝN
  143. Jensen-type inequalities for m-convex functions
  144. Special Issue on Problems, Methods and Applications of Nonlinear Analysis (Part III)
  145. The influence of the noise on the exact solutions of a Kuramoto-Sivashinsky equation
  146. Basic inequalities for statistical submanifolds in Golden-like statistical manifolds
  147. Global existence and blow up of the solution for nonlinear Klein-Gordon equation with variable coefficient nonlinear source term
  148. Hopf bifurcation and Turing instability in a diffusive predator-prey model with hunting cooperation
  149. Efficient fixed-point iteration for generalized nonexpansive mappings and its stability in Banach spaces
Downloaded on 7.12.2025 from https://www.degruyterbrill.com/document/doi/10.1515/math-2022-0060/html
Scroll to top button