We consider the following Schrödinger system
{−Δuj=k∑i=1βij|ui|3|uj|uj+λj|uj|q−2uj, inΩ,uj=0on∂Ω,j=1,⋯,k
where Ω⊂R3 is a bounded domain with smooth boundary. Assume 5<q<6,λj>0,βjj>0,j=1,⋯,k, βij=βji,i≠j,i,j=1,⋯,k. Note that the nonlinear coupling terms are of critical Sobolev growth in dimension 3. We prove that under an additional condition on the coupling matrix the problem has infinitely many sign-changing solutions. The result is obtained by combining the method of invariant sets of descending flow with the approach of using approximation of systems of subcritical growth.
Citation: Changmu Chu, Jiaquan Liu, Zhi-Qiang Wang. Sign-changing solutions for Schrödinger system with critical growth[J]. Electronic Research Archive, 2022, 30(1): 242-256. doi: 10.3934/era.2022013
[1] | Hui Guo, Tao Wang . A note on sign-changing solutions for the Schrödinger Poisson system. Electronic Research Archive, 2020, 28(1): 195-203. doi: 10.3934/era.2020013 |
[2] | Xian Zhang, Chen Huang . Existence and multiplicity of sign-changing solutions for supercritical quasi-linear Schrödinger equations. Electronic Research Archive, 2023, 31(2): 656-674. doi: 10.3934/era.2023032 |
[3] | Xia Su, Wen Guan, Xia Li . Least energy sign-changing solutions for Kirchhoff-Schrödinger-Poisson system on bounded domains. Electronic Research Archive, 2023, 31(5): 2959-2973. doi: 10.3934/era.2023149 |
[4] | Senli Liu, Haibo Chen . Existence and asymptotic behaviour of positive ground state solution for critical Schrödinger-Bopp-Podolsky system. Electronic Research Archive, 2022, 30(6): 2138-2164. doi: 10.3934/era.2022108 |
[5] | Xiaoyong Qian, Jun Wang, Maochun Zhu . Existence of solutions for a coupled Schrödinger equations with critical exponent. Electronic Research Archive, 2022, 30(7): 2730-2747. doi: 10.3934/era.2022140 |
[6] | Shujie Bai, Yueqiang Song, Dušan D. Repovš . On $ p $-Laplacian Kirchhoff-Schrödinger-Poisson type systems with critical growth on the Heisenberg group. Electronic Research Archive, 2023, 31(9): 5749-5765. doi: 10.3934/era.2023292 |
[7] | Hui Jian, Min Gong, Meixia Cai . Global existence, blow-up and mass concentration for the inhomogeneous nonlinear Schrödinger equation with inverse-square potential. Electronic Research Archive, 2023, 31(12): 7427-7451. doi: 10.3934/era.2023375 |
[8] | Guaiqi Tian, Hongmin Suo, Yucheng An . Multiple positive solutions for a bi-nonlocal Kirchhoff-Schr$ \ddot{\mathrm{o}} $dinger-Poisson system with critical growth. Electronic Research Archive, 2022, 30(12): 4493-4506. doi: 10.3934/era.2022228 |
[9] | Liangying Miao, Man Xu, Zhiqian He . Existence and multiplicity of positive solutions for one-dimensional $ p $-Laplacian problem with sign-changing weight. Electronic Research Archive, 2023, 31(6): 3086-3096. doi: 10.3934/era.2023156 |
[10] | Jiayi Fei, Qiongfen Zhang . On solutions for a class of Klein–Gordon equations coupled with Born–Infeld theory with Berestycki–Lions conditions on $ \mathbb{R}^3 $. Electronic Research Archive, 2024, 32(4): 2363-2379. doi: 10.3934/era.2024108 |
We consider the following Schrödinger system
{−Δuj=k∑i=1βij|ui|3|uj|uj+λj|uj|q−2uj, inΩ,uj=0on∂Ω,j=1,⋯,k
where Ω⊂R3 is a bounded domain with smooth boundary. Assume 5<q<6,λj>0,βjj>0,j=1,⋯,k, βij=βji,i≠j,i,j=1,⋯,k. Note that the nonlinear coupling terms are of critical Sobolev growth in dimension 3. We prove that under an additional condition on the coupling matrix the problem has infinitely many sign-changing solutions. The result is obtained by combining the method of invariant sets of descending flow with the approach of using approximation of systems of subcritical growth.
In this paper, we consider the Schrödinger system with critical growth
{−Δuj=k∑i=1βij|ui|3|uj|uj+λj|uj|q−2uj, inΩ,uj=0on∂Ω,j=1,⋯,k (P) |
where Ω⊂R3 is a bounded domain with smooth boundary. This type of coupled systems have applications in some physical problem. In physics literatures the signs of the coupling constants βij,i≠j being positive or negative determine the nature of the system being attractive or repulsive. We refer to [1,2,3,4,5,6,7] for further references on subcritical and critical problems therein. Our main result is the following.
Theorem 1.1. Assume 5<q<6, λj>0,j=1,⋯,k, βjj>0,j=1,⋯,k,βij=βji,i,j=1,⋯,k, and there exists β0>0 such that
k∑i,j=1βijξiξj≥β0|ξ|2forξ=(ξ1,⋯,ξk)∈Rk+. |
Then the problem (P) has infinitely many solutions with all components being sign-changing.
It is worth mentioning that our Theorem 1.1 allows some pairs of components to be attractive, and others repulsive.
Example 1.1. (attractive) βij≥0,i≠j,i,j=1,⋯,k.
Example 1.2. (repulsive) βij≤0,i≠j,i,j=1,⋯,k and the matrix B=(βij) is positive definite.
The problem (P) has a variational structure given by the functional
I(U)=12∫Ωk∑j=1|∇uj|2dx−16∫Ωk∑i,j=1βij|ui|3|uj|3dx−1q∫Ωk∑j=1λj|uj|qdx |
for U=(u1,⋯,uk)∈X=H10(Ω)×⋯×H10(Ω), the k-fold product of H10(Ω). In order to prove Theorem 1.1, we shall use a subcritical approximation scheme together with the method of invariant sets of descending flow, in particular the abstract theorem from [8,9]. We briefly outline our approaches here.
When we try to apply the abstract theorem to the functional I, we are faced with some difficulties. Firstly being in dimension 3 the problem (P) is of critical Sobolev growth, and the functional I fails to satisfy the Palais-Smale condition. From the classical work of [10] (see also for p-Laplacian in [11] and for coupled systems in [9,12]), using a subcritical approximation is an effective method to overcome this difficulty. Since we also need to study the nodal property, we shall use an alternative scheme of subcritical approximation as done in [13]. Our approach avoids passing to the limit of the subcritical problems and is easier to deal with nodal property of the solutions. Secondly in order to deal with nodal property of the solutions we employ the method of invariant sets of descending flow which has become a well developed method for constructing multiple nodal solutions, we refer [8,9,14,15,16,17,18,19,20] for further references therein. In particular we rely on the recent developments in [8,9]. To use the method of invariant set of descending flow one needs to construct certain invariant sets. This usually requires some additional property of the gradient flow (or a pseudo gradient flow). Our approximation approach also accommodates this issue well.
More precisely, we consider the perturbed functionals
I(ε)p(U)=12∫Ωk∑j=1|∇uj|2dx−12pgε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)−1q∫Ωk∑j=1λj|uj|qdx |
for U=(u1,⋯,uk)∈X, where 2<p<3,0<ε≤1 and gε is a smooth function satisfying
gε(t)=tfor0≤t≤1ε,gε(t)=cεt12fort≥2ε, | (1.1) |
here cε is a constant depending on ε. The critical points of I(ε)p will be used as approximate solutions of the problem (P) and it turns out that the approximate solutions converge to the solutions of the problem (P) as the parameters ε↓0,p↑3. Technically, we will first construct sign-changing critical points U of I(ε)p, then send ε to zero while holding p fixed to get sign-changing critical points U with ||U||∞<1ε for the functionals Ip defined by
Ip(U)=12∫Ωk∑j=1|∇uj|2dx−12p∫Ωk∑i,j=1βij|ui|p|uj|pdx−1q∫Ωk∑j=1λj|uj|qdx. |
Then using the profile decomposition of approximation solutions we obtain solutions of (P) by passing limit of p→3.
The paper is organized as follows. In Section 2 we will work on the perturbed functionals and construct multiple nodal solutions as approximating solutions to the original problem. Section 3 is devoted to the convergence analysis of the approximating solutions, then the proof of our main result follows.
First we give the exact definition of the function gε. Let φ be a smooth function such that φ(t)=1 for 0≤t≤1, φ(t)=12 for t≥2 and φ(t) is decreasing in t. Define g(t)=exp{∫t1φ(τ)τdτ} and, for ε>0, gε(t)=1εg(εt). Then gε satisfies (1.1) and
12gε(t)≤g′ε(t)t≤gε(t),g′ε(t)t12≤cεfort≥0. | (2.1) |
To construct multiple nodal solutions for the subcritical approximating problems we will make use of the following abstract theorem from [8,9]. In the following, γ(A) denotes the genus of a symmetric and closed subset A (see [21] for properties of the genus theory).
Theorem 2.1. Let X be a Banach space, f be an even C1-functional on X, A be an odd mapping from X to X, and Pj,Qj, j=1,⋯,k be open convex subsetsof X with Qj=−Pj. Denote W=k⋃j=1(Pj∪Qj), Σ=k⋂j=1(∂Pj∩∂Qj). Assume
(I1) f is an even C1-functional on X, and satisfies the Palais-Smale condition.
(I2) there exists c∗>0 such that
f(x)≥c∗,forx∈Σ. |
(A1) given b0>0,c0>0, there exists b=b(b0,c0) such that if |f(x)|≤c0,‖Df(x)‖≥b0, then
⟨Df(x),x−Ax⟩≥b‖x−Ax‖>0. |
(A2) A(∂Pj)⊂Pj,A(∂Qj)⊂Qj, j=1,⋯,k.
Introduce a sequence of families of subsets of X.
Γl={B|B⊂X,Bcompact,−B=Bandγ(B∩σ−1(Σ))≥lforσ∈Λ} |
Λ={σ|σ∈C(X,X),σodd,σ(Pj)⊂Pj,σ(Qj)⊂Qj,j=1,⋯,kandσ(x)=xiff(x)≤0}. |
Define
cl=infB∈Γlsupx∈B∖Wf(x). |
Assume
(Γ) Γl,l=1,2,⋯ are nonempty.
Then
(1) cl≥c∗,l=1,2,⋯ are critical values of f.
(2) c1≤c2≤⋯ and cl→+∞ as l→∞.
(3) The critical set K∗cl is nonempty, where
K∗c={x|x∈X∖W,f(x)=c,Df(x)=0}. |
(4) If cl=cl+1=⋯=cl+k−1 for some integer k, then γ(K∗cl)≥k.
(5) If X is a Hilbert space, f is a C2-functional and for every critical point x of f, D2f(x) is a Fredholm operator, thenthere exists x∈K∗cl with m∗(x,f)≥l, where m∗ is the augmented Morse index of x.
Lemma 2.1. The functional I(ε)p is of C2-class, satisfies the Palais-Smale condition and D2I(ε)p(U) is a Fredholm operator for everycritical point U of the functional I(ε)p.
Proof. Note that 2<p<q<6. Thus it is easy to verify that I(ε)p is a C2-functional. Moreover
⟨DI(ε)p(U),ϕ⟩=∫Ωk∑j=1∇uj∇φjdx−g′ε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)∫Ωk∑i,j=1βij|ui|p|uj|p−2ujφjdx−∫Ωk∑j=1λj|uj|q−2ujφjdxforϕ=(φ1,⋯,φk)∈X. | (2.2) |
We have
I(ε)p(U)−1p⟨DI(ε)p(U),U⟩=(12−1p)∫Ωk∑i,j=1|∇uj|2dx+1pg′ε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)∫Ωk∑i,j=1βij|ui|p|uj|pdx−12pgε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)+(1p−1q)∫Ωk∑j=1λj|uj|qdx≥(12−1p)∫Ωk∑j=1|∇uj|2dx=(12−1p)‖U‖2. | (2.3) |
In the above we have used the fact that g′ε(t)t≥12gε(t). By (2.3), any Palais-Smale sequence of I(ε)p is bounded in X. Since the functional I(ε)p is of subcritical growth, by a standard argument I(ε)p satisfies the Palais-Smale condition.
Let U be a critical point of I(ε)p. By the regularity theory, U is continuous on ˉΩ and therefore is uniformly bounded. Then the operator D2I(ε)p(U) is a compact perturbation of the Laplacian operator, hence a Fredholm operator.
Lemma 2.2. Denote β±ij=max(±βij, 0). Define a compact and odd operator A: U=(u1,⋯,uk)∈X↦V=(v1,⋯,vk)=AU∈X by the equations
∫Ω∇vj∇φjdx+g′ε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)∫Ωk∑i=1β−ij|ui|p|uj|p−2vjφjdx=g′ε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)∫Ωk∑i=1β+ij|ui|p|uj|p−2ujφjdx+λj∫Ω|uj|q−2ujφjdx | (2.4) |
for ϕ=(φ1,⋯,φk)∈X. Then the following property holds:if ‖I(ε)p(U)‖≤c0 and ‖DI(ε)p(U)‖≥b0>0, there exists b=b(b0,c0) such that
⟨DI(ε)p(U),U−AU⟩≥b‖U−AU‖>0. |
Proof. By (2.2) and (2.4), we have
⟨DI(ε)p(U),ϕ⟩=∫Ωk∑j=1∇(uj−vj)∇φjdx+g′ε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)∫Ωk∑i=1β−ij|ui|p|uj|p−2(uj−vj)φjdx | (2.5) |
for ϕ=(φ1,⋯,φk)∈X. Choose ϕ=U−V, we obtain
⟨DI(ε)p(U),U−V⟩=‖U−V‖2+g′ε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)∫Ωk∑i=1β−ij|ui|p|uj|p−2(uj−vj)2dx. |
Hence,
⟨DI(ε)p(U),U−V⟩≥‖U−V‖2 | (2.6) |
and
⟨DI(ε)p(U),U−V⟩≥g′ε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)∫Ωk∑i=1β−ij|ui|p|uj|p−2(uj−vj)2dx. | (2.7) |
It follows from (2.1), (2.5) and (2.7) that
|⟨DI(ε)p(U),ϕ⟩|≤‖U−V‖‖ϕ‖+g′ε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)(∫Ωk∑i=1β−ij|ui|p|uj|p−2φ2jdx)12⋅(∫Ωk∑i=1β−ij|ui|p|uj|p−2(uj−vj)2dx)12≤‖U−V‖‖ϕ‖+cg′ε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)‖U‖p−1L2p(Ω)‖ϕ‖L2p(Ω)⋅(∫Ωk∑i=1β−ij|ui|p|uj|p−2(uj−vj)2dx)12≤‖U−V‖‖ϕ‖+c(g′ε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)‖U‖pL2p(Ω))12‖U‖p−22L2p(Ω)‖ϕ‖L2p(Ω)⋅(g′ε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)∫Ωk∑i=1β−ij|ui|p|uj|p−2(uj−vj)2dx)12≤‖U−V‖‖ϕ‖+cβ−140√cε√⟨DI(ε)p(U),U−V⟩‖U‖p−22L2p(Ω)‖ϕ‖L2p(Ω), | (2.8) |
which implies that
‖⟨DI(ε)p(U)‖≤‖U−V‖+Cε‖U‖p−22L2p(Ω)(⟨DI(ε)p(U),U−V⟩)12. | (2.9) |
Choose s such that 2<s<p<q. Then we deduce from (2.1) and (2.5) that
I(ε)p(U)−1s⟨U−V,U⟩=I(ε)p(U)−1s⟨DI(ε)p(U),U⟩+1sg′ε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)∫Ωk∑i=1β−ij|ui|p|uj|p−2(uj−vj)ujdx=(12−1s)‖U‖2+1sg′ε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)∫Ωk∑i=1βij|ui|p|uj|pdx+1sg′ε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)∫Ωk∑i=1β−ij|ui|p|uj|p−2(uj−vj)ujdx−12pgε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)+(1s−1q)∫Ωk∑j=1λj|uj|qdx≥(12−1s)‖U‖2+(12s−12p)gε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)+1sg′ε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)∫Ωk∑i=1β−ij|ui|p|uj|p−2(uj−vj)ujdx. | (2.10) |
Notice that the matrix B=(βij) is positively definite, we have
k∑i,j=1β−ij|ui|p|uj|p≤C|U|2p≤Ck∑i,j=1βij|ui|p|uj|p. |
It implies from (2.1) that
g′ε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)∫Ωk∑i=1β−ij|ui|p|uj|pdx≤Cgε(∫Ωk∑i,j=1βij|ui|p|uj|pdx). | (2.11) |
From (2.7), (2.10) and (2.11), for sufficiently small σ>0, we obtain
(12−1s)‖U‖2+(12s−12p)gε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)≤I(ε)p(U)−1s⟨U−V,U⟩−1sg′ε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)∫Ωk∑i=1β−ij|ui|p|uj|p−2(uj−vj)ujdx≤I(ε)p(U)+1s|⟨U−V,U⟩|+C(g′ε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)∫Ωk∑i=1β−ij|ui|p|uj|pdx)12⋅(g′ε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)∫Ωk∑i=1β−ij|ui|p|uj|p−2(uj−vj)2dx)12≤|I(ε)p(U)|+1s|⟨U−V,U⟩|+C(gε(∫Ωk∑i,j=1βij|ui|p|uj|pdx))12√⟨DI(ε)p(U),U−V⟩≤|I(ε)p(U)|+C‖U−V‖2+C⟨DI(ε)p(U),U−V⟩+σ‖U‖2+σgε(∫Ωk∑i,j=1βij|ui|p|uj|pdx) |
Therefore,
gε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)≤C(|I(ε)p(U)|+‖U−V‖2+⟨DI(ε)p(U),U−V⟩). | (2.12) |
According to (1.1), there exists Cε>0 such that t12<Cε(1+gε(t)). Hence
‖U‖pL2p(Ω)≤C(∫Ωk∑i,j=1βij|ui|p|uj|pdx)12≤Cε(1+gε(∫Ωk∑i,j=1βij|ui|p|uj|pdx))≤Cε(1+|I(ε)p(U)|+‖U−V‖2+⟨DI(ε)p(U),U−V⟩). | (2.13) |
Combining (2.9) with (2.13), we obtain
‖⟨DI(ε)p(U)‖≤‖U−V‖+Cε(1+|I(ε)p(U)|+‖U−V‖2+⟨DI(ε)p(U),U−V⟩)p−22p(⟨DI(ε)p(U),U−V⟩)12. |
For σ>0 small enough, we have
(1+|I(ε)p(U)|+‖U−V‖2)p−22p(⟨DI(ε)p(U),U−V⟩)12≤C(1+|I(ε)p(U)|+‖U−V‖2)p−2p‖U−V‖+σ‖DI(ε)p(U)‖≤C(1+|I(ε)p(U)|p−2p+‖U−V‖2(p−2)p)‖U−V‖+σ‖DI(ε)p(U)‖ |
and
(⟨DI(ε)p(U),U−V⟩)p−22p(⟨DI(ε)p(U),U−V⟩)12≤(‖DI(ε)p(U)‖‖U−V‖)1−1p≤C‖U−V‖p−1+σ‖DI(ε)p(U)‖. |
By the above inequalities, we have
‖⟨DI(ε)p(U)‖≤Cε(1+|I(ε)p(U)|p−2p+‖U−V‖p−2)‖U−V‖. | (2.14) |
If ‖I(ε)p(U)‖≤c0 and ‖DI(ε)p(U)‖≥b0>0, we deduce from (2.13) that there exists b=b(b0,c0) such that ‖U−V‖>b. It follows from (2.6) that
⟨DI(ε)p(U),U−AU⟩≥b‖U−AU‖>0. |
That A is odd is obvious. The compactness of A follows the regularity theory and the subcritical growth.
Lemma 2.3. Let Pj,Qj,j=1,⋯,k be open convex subsets of X, defined by
Pj=Pj(δ)={U|U=(u1,⋯,uk)∈X,‖u−j‖L6(Ω)<δ} |
Qj=Qj(δ)={U|U=(u1,⋯,uk)∈X,‖u+j‖L6(Ω)<δ}. |
Then there exists a constant δ1>0 such that for 0<δ<δ1 it holds that
A(∂Pj)⊂Pj,A(∂Qj)⊂Qj,j=1,⋯,k. |
Proof. Choose ϕ=V+=(v+1,⋯,v+k) as test function in (2.4). Then we have
c‖v+j‖2L6(Ω)≤∫Ω∇vj∇v+jdx≤g′ε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)∫Ωk∑i=1β+ij|ui|p(u+j)p−1v+jdx+λj∫Ω(u+j)q−1v+jdx≤g′ε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)⋅c‖U‖pL2p(Ω)‖u+j‖p−1L2p(Ω)‖v+j‖L2p(Ω)+c‖u+j‖q−1Lq(Ω)‖v+j‖Lq(Ω)≤c′ε(‖u+j‖p−2L6(Ω)+‖u+j‖q−2L6(Ω))‖u+j‖L6(Ω)⋅‖v+j‖L6(Ω), | (2.15) |
where c′ε is a constant depending on ε but independent of p∈[52,3]. By (2.15) we have
‖v+j‖L6(Ω)≤c′ε(‖u+j‖p−2L6(Ω)+‖u+j‖q−2L6(Ω))‖u+j‖L6(Ω). | (2.16) |
Choose δ1 such that c′ε(δp−21+δq−21)≤12. Then for 0<δ<δ1 and U∈∂Qj we have ‖u+j‖L6(Ω)=δ and
‖v+j‖L6(Ω)≤c′ε(δp−2+δq−2)‖u+j‖L6(Ω)≤12‖u+j‖L6(Ω)=12δ. |
That is for U∈∂Qj, we have V=AU∈Qj and A(∂Qj)⊂Qj. Similarly A(∂Pj)⊂Pj,j=1,⋯,k.
Lemma 2.4. There exists δ2>0 such that for 0<δ<δ2 there exists c∗>0 independent of ε∈(0,1],p∈[2,3] such that
I(ε)p(U)≥c∗>0forU∈Σ. |
Proof.
I(ε)p=12∫Ωk∑j=1|∇uj|2dx−12pgε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)−1q∫Ωk∑j=1λj|uj|qdx≥12‖U‖2−c(‖U‖2pL2p(Ω)+‖U‖qLq(Ω))≥c1‖U‖2L6(Ω)−c2(‖U‖2pL6(Ω)+‖U‖qL6(Ω)). |
For U∈Σ=k⋂j=1(∂Pj∩∂Qj),
‖U‖6L6(Ω)=∫Ωk∑j=1((u+j)6+(u−j)6)dx=2kδ6. |
Hence
I(ε)p(U)≥c1‖U‖2L6(Ω)−c2(‖U‖2pL6(Ω)+‖U‖qL6(Ω))≥12c1‖U‖2L6(Ω)=12c1(6√2kδ)2:=c∗>0 |
provided c2((6√2kδ2)2p−2+(6√2kδ2)q−2)≤12c1 and 0<δ<δ2.
Now we define a sequence of critical values of the perturbed functional I(ε)p
cl(ε,p)=infB∈ΓlsupU∈B∖WI(ε)p(U),l=1,2,⋯ |
where W=k⋃j=1(Pj∪Qj) and for l=1,2,⋯
Γl={B|B⊂X,Bcompact,−B=B,γ(B∩σ−1(Σ))≥lforσ∈Λ}, |
Λ={σ|σ∈C(X,X),σoddσ(Pj)⊂Pj,σ(Qj)⊂Qj,j=1,⋯,kandσ(U)=UifI(ε)p(U)≤0}. |
Proposition 2.1. cl(ε,p),l=1,2,⋯ are critical values of the functional I(ε)p. There exists Ul(ε,p)∈X such that I(ε)p(Ul(ε,p))=cl(ε,p), DI(ε)p(Ul(ε,p))=0, Ul(ε,p) is sign-changing and the augmented Morse indexm∗(Ul(ε,p),I(ε)p)≥l. Moreover there exists a constant Ll, independent of ε,p, such that
I(ε)p(Ul(ε,p))=cl(ε,p)≤Lpε∈(0,1],p∈(2,3). |
Proof. We apply Theorem 2.1 to our functional I(ε)p. We have verified the conditions (I1)(Lemma 2.1), (I2)(Lemma 2.4), (A1)(Lemma 2.2) and (A2)(Lemma 2.3). We need only to verify the condition Γ. Denote n=l+k. Choose nk functions vi∈C∞0(Ω),i=1,⋯,nk with disjoint supports. Denote
Fl={U|U=(n∑i=1tivi,2n∑i=n+1tivi,⋯,nk∑i=n(k−1)+1tivi)∈X,t=(t1,t2,⋯,tnk)∈Rnk,|t|≤R}. |
By Lemma 4.2 in [9] for R sufficiently large Fl∈Γl, Γl is nonempty. Now we have
cl(ε,p)≤supU∈FlI(ε)p(U)≤supU∈ElJ(U):=Ll, |
where
J(U)=12∫Ωk∑j=1|∇uj|2dx−1q∫Ωk∑j=1λj|uj|qdx,U=(u1,⋯,uk)∈X, |
El={U|U=(n∑i=1tivi,2n∑i=n+1tivi,⋯,nk∑i=n(k−1)+1tivi)∈Xt=(t1,t2,⋯,tnk)∈Rnk}. |
As we have mentioned that the critical points of the perturbed functional I(ε)p will be used as approximate solutions of the original problem (P). Now we prove that these approximate solutions converge to solutions of the original problem. More precisely, we show for any given integer k, we can find ϵ>0 small so that the functional I(ε)p has k nodal critical points whose L∞ norm all less than 1ε (therefore they are critical points of the functional Ip). Then we send p to 3 to get solutions of the original problem.
Lemma 3.1. Assume that U∈X satisfies I(ε)p(U)≤L,DI(ε)p(U)=0, where L is independent of ε,p. Then there exists a constant ˉε=ˉε(L) such that if 0<ε<ˉε, Ip(U)=I(ε)p(U),DIp(U)=DI(ε)p(U)=0, U is a critical point of Ip.
Proof. By (2.3), we have
L≥I(ε)p(U)=I(ε)p(U)−1p⟨DI(ε)p(U),U⟩≥(12−1p)‖U‖2. |
There exists a constant M, independent of ε,p, such that
‖U‖2≤M,∫Ωk∑i,j=1βij|ui|p|uj|pdx≤M. |
Choose ˉε=12M. Then for 0<ε<ˉε,
gε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)=∫Ωk∑i,j=1βij|ui|p|uj|pdx,g′ε(∫Ωk∑i,j=1βij|ui|p|uj|pdx)=1. |
Hence for 0<ε<ˉε, Ip(U)=I(ε)p(U), DIp(U)=DI(ε)p(U)=0.
Lemma 3.2. Assume pn∈(2,3], pn→3, Un∈X, n=1,2,⋯ such that Ipn(Un)≤L,DIp(Un)=0, where L is independent of p, and Unis sign-changing. Then Un is bounded in X. Assume Un⇀U in X. Then Un→U in X, I(U)≤L,DI(U)=0 and U is sign-changing.
Proof. Again we have
L≥Ipn(Un)=Ipn(Un)−1pn⟨DIpn(Un),Un⟩≥(12−12pn)‖Un‖2≥14‖Un‖2. |
So Un is bounded in X. Assume Un⇀U in X. We have the following profile decomposition [22]
Un=U+∑k∈Λσ12n,kVk(σn,k(⋅−xn,k))+Rn | (3.1) |
where Vk∈D=D(R3),Rn∈D,xn,k∈¯Ω,σn,k→+∞, Rn→0 in L6(Ω) as n→∞.
Assume σn=σn,1=min{σn,k|k∈Λ},xn=xn,1. The following claim can be proved as in [9,10,11].
Claim. There exist positive constant c,¯c such that
|Un(x)|≤cforx∈An,∫An|∇Un|2dx≤cσ−12n | (3.2) |
where An is called a safe region and defined by
An={x|x∈R3,(ˉc+2)σ−12n<|x−xn|<(ˉc+3)σ−12n}. |
Let Un=(u1,⋯,uk)∈X be a critical point of Ipn. The following local Pohožaev identity holds (e.g., [9]):
(32pn−12)∫Dnk∑j=1|Duj|2dx+(3q−32pn)∫Dnλj|uj|pdx=12∫Dnk∑i,j=1|∇uj|2(x−x∗,∇η)dx−∫Dnk∑j=1(∇uj,∇η)dx−∫Dnk∑j=1(∇uj,x−x∗)(∇uj,∇η)dx−32pn∫Dnk∑j=1(∇uj,∇η)ujdx−∫Dn(1qk∑j=1λj|uj|q+12pnk∑i,j=1βij|ui|pn|uj|pn)(x−x∗,∇η)dx+12∫∂eDnk∑j=1|∇uj|2(x−x∗,n)ηdσ | (3.3) |
where Dn=B(ˉc+3)σ−12n(xn), ∂eDn=∂Dn∩∂Ω, n is the outward normal to ∂Ω, x∗∈RN,η∈C∞0(R3) such that η(x)=1 for |x−x∗|≤(ˉc+2)σ−12n, η(x)=0 for |x−x∗|≥(ˉc+3)σ−12n and |∇η|≤2σ12n.
Choose x∗ such that |x∗−x|≤(ˉc+8)σ−12n and (x−x∗,n)≤0 for all x∈∂eDn. If ∂eDn=∅ we simply choose x∗=xn. With this choice of x∗ and the fact 2pn≤6 we have
(Nq−N2pn)∫Dnk∑j=1λj|uj|qηdx≤12∫Dnk∑j=1|∇uj|2(x−x∗,∇η)dx−∫Dnk∑j=1(∇uj,x−x∗)(∇uj,∇η)dx−N2pn∫Dnk∑j=1(∇uj,∇η)ujdx−∫Dn(1qk∑j=1λj|uj|q+12pnk∑i,j=1βij|ui|pn|uj|pn)(x−x∗,∇η)dx. | (3.4) |
The integrals of the right hand side of (3.4) are taken over the domain An due to the fact that ∇η=0 outside An. Hence by the claim (3.2), we have
RHSof(3.4)≤cσ−12n. |
For the left hand side of (3.4), we have, keeping the profile decomposition (3.2) in mind
LHSof(3.4)=(Nq−N2pn)∫Dnk∑j=1λj|uj|qηdx≥c∫Dn|Un|qdx≥cσq2−3n∫|y|≤L|σ−12nUn(σ−1ny+xn)|qdx≥cσq2−3n. |
In the above we assume σ−12nUn(σ−1n⋅+xn)⇀V in D and choose L>0 such that ∫|y|≤L|V|qdx>0. Because q>5 we arrive at a contradiction for n large in
σq2−3n≤cσ−12n. |
Hence the index set Λ in the profile decomposition (3.1) is empty and Un→U in L6(Ω), which implies that Un→U in X due to the fact DIpn(Un)=0. Therefore I(U)=limn→∞Ipn(Un)≤L and DI(U)=limn→∞DIpn(Un)=0.
Finally we prove that U is sign-changing. Denote Un=(u1n,⋯,ukn), U=(u1,⋯,uk). We have
∫Ω∇ujn∇φjdx=∫Ωk∑i=1βij|uin|pn|ujn|pn−2ujnφjdx+λj∫Ω|ujn|q−2ujnφjdx,φj∈H10(Ω). |
Choosing φj=u+jn, we have
c‖u+jn‖2L6(Ω)≤∫Ω∇ujn∇u+jndx=∫Ωk∑i=1βij|uin|pn|ujn|pn−2ujnu+jndx+λj∫Ω|ujn|q−2ujnu+jndx≤∫Ωk∑i=1βij|uin|pn(u+jn)pndx+λj∫Ω(u+jn)qdx≤‖Un‖pnL2pn(Ω)‖u+jn‖pnL2pn(Ω)+λj‖u+jn‖qLq(Ω)≤(‖Un‖2pn−52+‖Un‖q−52)‖u+jn‖52L6(Ω)≤c(L)‖u+jn‖52L6(Ω), |
in which we used that ‖Un‖2 is bounded by 4L. Hence there exists δ>0 such that ‖u+jn‖L6(Ω)≥δ and ‖uj‖L6(Ω)=limn→∞‖u+jn‖L6(Ω)≥δ>0. Similarly ‖u−j‖L6(Ω)≥δ>0,j=1,⋯,k and we have U=(u1,⋯,uk) is sign-changing.
Proof of Theorem 1.1. First, obviously functions in X∖W are sign-changing. Given an integer l, by Proposition 2.1 the functional I(ε)p,0<ε≤1,2<p<3 has a sign-changing critical point Ul(ε,p) with the augmented Morse index m∗(Ul(ε,l),I(ε)p)≥l. Moreover, there exists a constant Ll, independent of ε,p, such that I(ε)p(Ul(ε,p))≤Ll.
By Lemma 3.1 there exists ˉε=ˉε(Ll), independent of p, such that 0<ε<ˉε,Ip(Ul(ε,p))=I(ε)p(Ul(ε,p))≤Ll, DIp(Ul(ε,p))=DI(ε)p(Ul(ε,p))=0. Denote Ul(p)=Ul(ε,p). Then Ul(p) is a sign-changing critical point of the functional Ip with the augmented Morse index m∗(Ul(p),Ip)≥l. Moreover Ip(Ul(p))≤Lp for 2<p<3.
Choose pn∈(2,3),pn→3. By Lemma 3.2, Ul(pn) is bounded in X. Assume Ul(pn)⇀Ul in X. Then Ul(pn)→Ul in X, I(Ul)≤Ll,DI(Ul)=0, Ul is sign-changing, and the augmented Morse index
m∗(Ul,I)≥¯limn→∞m∗(Ul(pn),Ipn)≥l. |
Ul is a sign-changing critical point of the functional I with m∗(Ul,I)≥l. Since the integer l is arbitrary, I has infinitely many sign-changing critical points, that is the problem (P) has infinitely many sign-changing solutions. Finally we prove I(Ul)→+∞ as l→∞. Otherwise I(Ul)≤L,DI(Ul)=0. By Lemma 3.2 Ul is bounded in X. Assume Uln⇀U in X as ln→∞. Then by Lemma 3.2, Uln→U in X, DI(U)=0. Therefore
+∞>m∗(U,I)≥¯limn→∞m∗(Uln,I)≥limn→∞ln=+∞, |
we arrive at a contradiction.
The work is supported by NSFC (11771324, 11831009, 11861021, 12071438).
The authors declare there is no conflict of interest.
[1] | T. Bartsch, Z.-Q. Wang, Note on ground states of nonlinear Schrödinger systems, Partial Differ. Equ., 3 (2006), 200–207. |
[2] |
Z. Chen, W. Zou, On an elliptic problem with critical exponent and Hardy potential, J. Differ. Equ., 252 (2012), 969–987. https://doi.org/10.1016/j.jde.2011.09.042 doi: 10.1016/j.jde.2011.09.042
![]() |
[3] |
Z. Chen, W. Zou, Ground states for a system of Schrödinger equations with critical exponent, J. Funct. Anal., 262 (2012), 3091–3107. https://doi.org/10.1016/j.jfa.2012.01.001 doi: 10.1016/j.jfa.2012.01.001
![]() |
[4] |
Z. Chen, C.-S. Lin, W. Zou, Infinitely many sign-changing and semi-nodal solutions for a nonlinear Schrödinger system, Ann. Sc. Norm. Super. Pisa Cl. Sci., 15 (2016), 859–897. https://doi.org/10.2422/20362145.201401_002 doi: 10.2422/20362145.201401_002
![]() |
[5] |
T.-C. Lin, J. Wei, Ground state of N coupled nonlinear Schrödinger equations in Rn,n≤3, Comm. Math. Phys. 255 (2005), 629–653. https://doi.org/10.1007/s002200051313x doi: 10.1007/s002200051313x
![]() |
[6] |
Z. Liu, Z.-Q. Wang, Multiple bound states of nonlinear Schrödinger systems, Comm. Math. Phys., 282 (2008), 721–731. https://doi.org/10.1007/s002200080546x doi: 10.1007/s002200080546x
![]() |
[7] |
Z. Liu, Z.-Q. Wang, Ground States and Bound States of a Nonlinear Schrödinger System, Adv. Nonlinear Stud., 10 (2010), 175–193. https://doi.org/10.1515/ans20100109 doi: 10.1515/ans20100109
![]() |
[8] |
J. Liu, X. Liu, Z.-Q. Wang, Multiple mixed states of nodal solutions for nonlinear Schrödinger systems, Calc. Var. Partial Differ. Equ., 52 (2015), 565–586. https://doi.org/10.1007/s005260140724y doi: 10.1007/s005260140724y
![]() |
[9] |
J. Liu, X. Liu, Z.-Q. Wang, Sign-changing solutions for coupled nonlinear Schrödinger equations with critical growth, J. Differ. Equ., 261 (2016), 7194–7236. https://doi.org/10.1016/j.jde.2016.09.018 doi: 10.1016/j.jde.2016.09.018
![]() |
[10] | G. Devillanova, S. Solimini, Concentrations estimates and multiple solutions to elliptic problems at critical growth, Adv. Differ. Equ., 7 (2002), 1257–1280. |
[11] |
D. Cao, S. Peng, S. Yan, Infinitely many solutions for p-Laplacian equation involving critical Sobolev growth, J. Funct. Anal., 262 (2012), 2861–2902. https://doi.org/10.1016/j.jfa.2012.01.006 doi: 10.1016/j.jfa.2012.01.006
![]() |
[12] |
Z. Chen, C.-S. Lin, W. Zou, Sign-changing solutions and phase separation for an elliptic system with critical exponent, Comm. Partial Differ. Equ., 39 (2014), 1827–1859. https://doi.org/10.1080/03605302.2014.908391 doi: 10.1080/03605302.2014.908391
![]() |
[13] |
J. Zhao, X. Liu, J. Liu, p-Laplacian equations in RN with finite potential via truncation method, the critical case, J. Math. Anal. Appl., 455 (2017), 58–88. https://doi.org/10.1016/j.jmaa.2017.03.085 doi: 10.1016/j.jmaa.2017.03.085
![]() |
[14] |
T. Bartsch, Critical point theory on partially ordered Hilbert spaces, J. Funct. Anal., 186 (2001), 117–152. https://doi.org/10.1006/jfan.2001.3789 doi: 10.1006/jfan.2001.3789
![]() |
[15] |
T. Bartsch, Z.-Q. Wang, On the existence of sign changing solutions for semilinear Dirichlet problems, Topol. Methods Nonlinear Anal., 7 (1996), 115–131. https://doi.org/10.12775/TMNA.1996.005 doi: 10.12775/TMNA.1996.005
![]() |
[16] |
T. Bartsch, K.-C. Chang, Z.-Q. Wang, On the Morse indices of sign changing solutions of nonlinear elliptic problems, Math. Z., 233 (2000), 655–677. https://doi.org/10.1007/s002090050492 doi: 10.1007/s002090050492
![]() |
[17] |
T. Bartsch, Z. Liu, T. Weth, Sign changing solutions of superlinear Schrödinger equations, Commun. Partial Differ. Equ., 29 (2004), 25–42. https://doi.org/10.1081/PDE-120028842 doi: 10.1081/PDE-120028842
![]() |
[18] |
T. Bartsch, Z. Liu, T. Weth, Nodal solutions of a p-Laplacian equation, Proc. Lond. Math. Soc., 91 (2005), 129–152. https://doi.org/10.1112/S0024611504015187 doi: 10.1112/S0024611504015187
![]() |
[19] |
S. Li, Z.-Q. Wang, Ljusternik-Schnirelman theory in partially ordered Hilbert spaces, Trans. Amer. Math. Soc., 354 (2002), 3207–3227. https://doi.org/10.1090/S0002994702030313 doi: 10.1090/S0002994702030313
![]() |
[20] |
Z. Liu, J. Sun, Invariant sets of descending flow in critical point theory with applications to nonlinear differential equations, J. Differ.l Equ., 172 (2001), 257–299. https://doi.org/10.1006/jdeq.2000.3867 doi: 10.1006/jdeq.2000.3867
![]() |
[21] | P. Rabinowitz, Minimax Methods in Critical Point Theory with Applications to Differential Equations. CBMS Regional Conf. Ser. in Math., vol. 65. American Mathematical Society, Providence, 1986. https://doi.org/10.1090/cbms/065 |
[22] | K. Tintarev, K.-H. Fieseler, Concentration compactness. Functional-analytic grounds and applications. Imperial College Press, London, 2007. https://doi.org/10.1142/p456 |