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Research article Special Issues

Sign-changing solutions for Schrödinger system with critical growth

  • We consider the following Schrödinger system

    {Δuj=ki=1βij|ui|3|uj|uj+λj|uj|q2uj,   inΩ,uj=0onΩ,j=1,,k

    where ΩR3 is a bounded domain with smooth boundary. Assume 5<q<6,λj>0,βjj>0,j=1,,k, βij=βji,ij,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

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  • We consider the following Schrödinger system

    {Δuj=ki=1βij|ui|3|uj|uj+λj|uj|q2uj,   inΩ,uj=0onΩ,j=1,,k

    where ΩR3 is a bounded domain with smooth boundary. Assume 5<q<6,λj>0,βjj>0,j=1,,k, βij=βji,ij,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=ki=1βij|ui|3|uj|uj+λj|uj|q2uj,   inΩ,uj=0onΩ,j=1,,k                 (P)

    where ΩR3 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,ij 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

    ki,j=1βijξiξjβ0|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) βij0,ij,i,j=1,,k.

    Example 1.2. (repulsive) βij0,ij,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)=12Ωkj=1|uj|2dx16Ωki,j=1βij|ui|3|uj|3dx1qΩkj=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)=12Ωkj=1|uj|2dx12pgε(Ωki,j=1βij|ui|p|uj|pdx)1qΩkj=1λj|uj|qdx

    for U=(u1,,uk)X, where 2<p<3,0<ε1 and gε is a smooth function satisfying

    gε(t)=tfor0t1ε,gε(t)=cεt12fort2ε, (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 ε0,p3. 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)=12Ωkj=1|uj|2dx12pΩki,j=1βij|ui|p|uj|pdx1qΩkj=1λj|uj|qdx.

    Then using the profile decomposition of approximation solutions we obtain solutions of (P) by passing limit of p3.

    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 0t1, φ(t)=12 for t2 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)gε(t)tgε(t),gε(t)t12cεfort0. (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=kj=1(PjQj), Σ=kj=1(PjQj). 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,forxΣ.

    (A1) given b0>0,c0>0, there exists b=b(b0,c0) such that if |f(x)|c0,Df(x)b0, then

    Df(x),xAxbxAx>0.

    (A2) A(Pj)Pj,A(Qj)Qj, j=1,,k.

    Introduce a sequence of families of subsets of X.

    Γl={B|BX,Bcompact,B=Bandγ(Bσ1(Σ))lforσΛ}
    Λ={σ|σC(X,X),σodd,σ(Pj)Pj,σ(Qj)Qj,j=1,,kandσ(x)=xiff(x)0}.

    Define

    cl=infBΓlsupxBWf(x).

    Assume

    (Γ) Γl,l=1,2, are nonempty.

    Then

    (1) clc,l=1,2, are critical values of f.

    (2) c1c2 and cl+ as l.

    (3) The critical set Kcl is nonempty, where

    Kc={x|xXW,f(x)=c,Df(x)=0}.

    (4) If cl=cl+1==cl+k1 for some integer k, then γ(Kcl)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 xKcl 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=Ωkj=1ujφjdxgε(Ωki,j=1βij|ui|p|uj|pdx)Ωki,j=1βij|ui|p|uj|p2ujφjdxΩkj=1λj|uj|q2ujφjdxforϕ=(φ1,,φk)X. (2.2)

    We have

    I(ε)p(U)1pDI(ε)p(U),U=(121p)Ωki,j=1|uj|2dx+1pgε(Ωki,j=1βij|ui|p|uj|pdx)Ωki,j=1βij|ui|p|uj|pdx12pgε(Ωki,j=1βij|ui|p|uj|pdx)+(1p1q)Ωkj=1λj|uj|qdx(121p)Ωkj=1|uj|2dx=(121p)U2. (2.3)

    In the above we have used the fact that gε(t)t12gε(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)XV=(v1,,vk)=AUX by the equations

    Ωvjφjdx+gε(Ωki,j=1βij|ui|p|uj|pdx)Ωki=1βij|ui|p|uj|p2vjφjdx=gε(Ωki,j=1βij|ui|p|uj|pdx)Ωki=1β+ij|ui|p|uj|p2ujφjdx+λjΩ|uj|q2ujφjdx (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),UAUbUAU>0.

    Proof. By (2.2) and (2.4), we have

    DI(ε)p(U),ϕ=Ωkj=1(ujvj)φjdx+gε(Ωki,j=1βij|ui|p|uj|pdx)Ωki=1βij|ui|p|uj|p2(ujvj)φjdx (2.5)

    for ϕ=(φ1,,φk)X. Choose ϕ=UV, we obtain

    DI(ε)p(U),UV=UV2+gε(Ωki,j=1βij|ui|p|uj|pdx)Ωki=1βij|ui|p|uj|p2(ujvj)2dx.

    Hence,

    DI(ε)p(U),UVUV2 (2.6)

    and

    DI(ε)p(U),UVgε(Ωki,j=1βij|ui|p|uj|pdx)Ωki=1βij|ui|p|uj|p2(ujvj)2dx. (2.7)

    It follows from (2.1), (2.5) and (2.7) that

    |DI(ε)p(U),ϕ|UVϕ+gε(Ωki,j=1βij|ui|p|uj|pdx)(Ωki=1βij|ui|p|uj|p2φ2jdx)12(Ωki=1βij|ui|p|uj|p2(ujvj)2dx)12UVϕ+cgε(Ωki,j=1βij|ui|p|uj|pdx)Up1L2p(Ω)ϕL2p(Ω)(Ωki=1βij|ui|p|uj|p2(ujvj)2dx)12UVϕ+c(gε(Ωki,j=1βij|ui|p|uj|pdx)UpL2p(Ω))12Up22L2p(Ω)ϕL2p(Ω)(gε(Ωki,j=1βij|ui|p|uj|pdx)Ωki=1βij|ui|p|uj|p2(ujvj)2dx)12UVϕ+cβ140cεDI(ε)p(U),UVUp22L2p(Ω)ϕL2p(Ω), (2.8)

    which implies that

    DI(ε)p(U)UV+CεUp22L2p(Ω)(DI(ε)p(U),UV)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)1sUV,U=I(ε)p(U)1sDI(ε)p(U),U+1sgε(Ωki,j=1βij|ui|p|uj|pdx)Ωki=1βij|ui|p|uj|p2(ujvj)ujdx=(121s)U2+1sgε(Ωki,j=1βij|ui|p|uj|pdx)Ωki=1βij|ui|p|uj|pdx+1sgε(Ωki,j=1βij|ui|p|uj|pdx)Ωki=1βij|ui|p|uj|p2(ujvj)ujdx12pgε(Ωki,j=1βij|ui|p|uj|pdx)+(1s1q)Ωkj=1λj|uj|qdx(121s)U2+(12s12p)gε(Ωki,j=1βij|ui|p|uj|pdx)+1sgε(Ωki,j=1βij|ui|p|uj|pdx)Ωki=1βij|ui|p|uj|p2(ujvj)ujdx. (2.10)

    Notice that the matrix B=(βij) is positively definite, we have

    ki,j=1βij|ui|p|uj|pC|U|2pCki,j=1βij|ui|p|uj|p.

    It implies from (2.1) that

    gε(Ωki,j=1βij|ui|p|uj|pdx)Ωki=1βij|ui|p|uj|pdxCgε(Ωki,j=1βij|ui|p|uj|pdx). (2.11)

    From (2.7), (2.10) and (2.11), for sufficiently small σ>0, we obtain

    (121s)U2+(12s12p)gε(Ωki,j=1βij|ui|p|uj|pdx)I(ε)p(U)1sUV,U1sgε(Ωki,j=1βij|ui|p|uj|pdx)Ωki=1βij|ui|p|uj|p2(ujvj)ujdxI(ε)p(U)+1s|UV,U|+C(gε(Ωki,j=1βij|ui|p|uj|pdx)Ωki=1βij|ui|p|uj|pdx)12(gε(Ωki,j=1βij|ui|p|uj|pdx)Ωki=1βij|ui|p|uj|p2(ujvj)2dx)12|I(ε)p(U)|+1s|UV,U|+C(gε(Ωki,j=1βij|ui|p|uj|pdx))12DI(ε)p(U),UV|I(ε)p(U)|+CUV2+CDI(ε)p(U),UV+σU2+σgε(Ωki,j=1βij|ui|p|uj|pdx)

    Therefore,

    gε(Ωki,j=1βij|ui|p|uj|pdx)C(|I(ε)p(U)|+UV2+DI(ε)p(U),UV). (2.12)

    According to (1.1), there exists Cε>0 such that t12<Cε(1+gε(t)). Hence

    UpL2p(Ω)C(Ωki,j=1βij|ui|p|uj|pdx)12Cε(1+gε(Ωki,j=1βij|ui|p|uj|pdx))Cε(1+|I(ε)p(U)|+UV2+DI(ε)p(U),UV). (2.13)

    Combining (2.9) with (2.13), we obtain

    DI(ε)p(U)UV+Cε(1+|I(ε)p(U)|+UV2+DI(ε)p(U),UV)p22p(DI(ε)p(U),UV)12.

    For σ>0 small enough, we have

    (1+|I(ε)p(U)|+UV2)p22p(DI(ε)p(U),UV)12C(1+|I(ε)p(U)|+UV2)p2pUV+σDI(ε)p(U)C(1+|I(ε)p(U)|p2p+UV2(p2)p)UV+σDI(ε)p(U)

    and

    (DI(ε)p(U),UV)p22p(DI(ε)p(U),UV)12(DI(ε)p(U)UV)11pCUVp1+σDI(ε)p(U).

    By the above inequalities, we have

    DI(ε)p(U)Cε(1+|I(ε)p(U)|p2p+UVp2)UV. (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 UV>b. It follows from (2.6) that

    DI(ε)p(U),UAUbUAU>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,ujL6(Ω)<δ}
    Qj=Qj(δ)={U|U=(u1,,uk)X,u+jL6(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

    cv+j2L6(Ω)Ωvjv+jdxgε(Ωki,j=1βij|ui|p|uj|pdx)Ωki=1β+ij|ui|p(u+j)p1v+jdx+λjΩ(u+j)q1v+jdxgε(Ωki,j=1βij|ui|p|uj|pdx)cUpL2p(Ω)u+jp1L2p(Ω)v+jL2p(Ω)+cu+jq1Lq(Ω)v+jLq(Ω)cε(u+jp2L6(Ω)+u+jq2L6(Ω))u+jL6(Ω)v+jL6(Ω), (2.15)

    where cε is a constant depending on ε but independent of p[52,3]. By (2.15) we have

    v+jL6(Ω)cε(u+jp2L6(Ω)+u+jq2L6(Ω))u+jL6(Ω). (2.16)

    Choose δ1 such that cε(δp21+δq21)12. Then for 0<δ<δ1 and UQj we have u+jL6(Ω)=δ and

    v+jL6(Ω)cε(δp2+δq2)u+jL6(Ω)12u+jL6(Ω)=12δ.

    That is for UQj, we have V=AUQj 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>0forUΣ.

    Proof.

    I(ε)p=12Ωkj=1|uj|2dx12pgε(Ωki,j=1βij|ui|p|uj|pdx)1qΩkj=1λj|uj|qdx12U2c(U2pL2p(Ω)+UqLq(Ω))c1U2L6(Ω)c2(U2pL6(Ω)+UqL6(Ω)).

    For UΣ=kj=1(PjQj),

    U6L6(Ω)=Ωkj=1((u+j)6+(uj)6)dx=2kδ6.

    Hence

    I(ε)p(U)c1U2L6(Ω)c2(U2pL6(Ω)+UqL6(Ω))12c1U2L6(Ω)=12c1(62kδ)2:=c>0

    provided c2((62kδ2)2p2+(62kδ2)q2)12c1 and 0<δ<δ2.

    Now we define a sequence of critical values of the perturbed functional I(ε)p

    cl(ε,p)=infBΓlsupUBWI(ε)p(U),l=1,2,

    where W=kj=1(PjQj) and for l=1,2,

    Γl={B|BX,Bcompact,B=B,γ(Bσ1(Σ))lforσΛ},
    Λ={σ|σC(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 viC0(Ω),i=1,,nk with disjoint supports. Denote

    Fl={U|U=(ni=1tivi,2ni=n+1tivi,,nki=n(k1)+1tivi)X,t=(t1,t2,,tnk)Rnk,|t|R}.

    By Lemma 4.2 in [9] for R sufficiently large FlΓl, Γl is nonempty. Now we have

    cl(ε,p)supUFlI(ε)p(U)supUElJ(U):=Ll,

    where

    J(U)=12Ωkj=1|uj|2dx1qΩkj=1λj|uj|qdx,U=(u1,,uk)X,
    El={U|U=(ni=1tivi,2ni=n+1tivi,,nki=n(k1)+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 UX 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

    LI(ε)p(U)=I(ε)p(U)1pDI(ε)p(U),U(121p)U2.

    There exists a constant M, independent of ε,p, such that

    U2M,Ωki,j=1βij|ui|p|uj|pdxM.

    Choose ˉε=12M. Then for 0<ε<ˉε,

    gε(Ωki,j=1βij|ui|p|uj|pdx)=Ωki,j=1βij|ui|p|uj|pdx,gε(Ωki,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], pn3, UnX, 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 UnU in X. Then UnU in X, I(U)L,DI(U)=0 and U is sign-changing.

    Proof. Again we have

    LIpn(Un)=Ipn(Un)1pnDIpn(Un),Un(1212pn)Un214Un2.

    So Un is bounded in X. Assume UnU in X. We have the following profile decomposition [22]

    Un=U+kΛσ12n,kVk(σn,k(xn,k))+Rn (3.1)

    where VkD=D(R3),RnD,xn,k¯Ω,σn,k+, Rn0 in L6(Ω) as n.

    Assume σn=σn,1=min{σn,k|kΛ},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)|cforxAn,An|Un|2dxcσ12n (3.2)

    where An is called a safe region and defined by

    An={x|xR3,(ˉc+2)σ12n<|xxn|<(ˉc+3)σ12n}.

    Let Un=(u1,,uk)X be a critical point of Ipn. The following local Pohožaev identity holds (e.g., [9]):

    (32pn12)Dnkj=1|Duj|2dx+(3q32pn)Dnλj|uj|pdx=12Dnki,j=1|uj|2(xx,η)dxDnkj=1(uj,η)dxDnkj=1(uj,xx)(uj,η)dx32pnDnkj=1(uj,η)ujdxDn(1qkj=1λj|uj|q+12pnki,j=1βij|ui|pn|uj|pn)(xx,η)dx+12eDnkj=1|uj|2(xx,n)ηdσ (3.3)

    where Dn=B(ˉc+3)σ12n(xn), eDn=DnΩ, n is the outward normal to Ω, xRN,ηC0(R3) such that η(x)=1 for |xx|(ˉc+2)σ12n, η(x)=0 for |xx|(ˉc+3)σ12n and |η|2σ12n.

    Choose x such that |xx|(ˉc+8)σ12n and (xx,n)0 for all xeDn. If eDn= we simply choose x=xn. With this choice of x and the fact 2pn6 we have

    (NqN2pn)Dnkj=1λj|uj|qηdx12Dnkj=1|uj|2(xx,η)dxDnkj=1(uj,xx)(uj,η)dxN2pnDnkj=1(uj,η)ujdxDn(1qkj=1λj|uj|q+12pnki,j=1βij|ui|pn|uj|pn)(xx,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)cσ12n.

    For the left hand side of (3.4), we have, keeping the profile decomposition (3.2) in mind

    LHSof(3.4)=(NqN2pn)Dnkj=1λj|uj|qηdxcDn|Un|qdxcσq23n|y|L|σ12nUn(σ1ny+xn)|qdxcσq23n.

    In the above we assume σ12nUn(σ1n+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

    σq23ncσ12n.

    Hence the index set Λ in the profile decomposition (3.1) is empty and UnU in L6(Ω), which implies that UnU in X due to the fact DIpn(Un)=0. Therefore I(U)=limnIpn(Un)L and DI(U)=limnDIpn(Un)=0.

    Finally we prove that U is sign-changing. Denote Un=(u1n,,ukn), U=(u1,,uk). We have

    Ωujnφjdx=Ωki=1βij|uin|pn|ujn|pn2ujnφjdx+λjΩ|ujn|q2ujnφjdx,φjH10(Ω).

    Choosing φj=u+jn, we have

    cu+jn2L6(Ω)Ωujnu+jndx=Ωki=1βij|uin|pn|ujn|pn2ujnu+jndx+λjΩ|ujn|q2ujnu+jndxΩki=1βij|uin|pn(u+jn)pndx+λjΩ(u+jn)qdxUnpnL2pn(Ω)u+jnpnL2pn(Ω)+λju+jnqLq(Ω)(Un2pn52+Unq52)u+jn52L6(Ω)c(L)u+jn52L6(Ω),

    in which we used that Un2 is bounded by 4L. Hence there exists δ>0 such that u+jnL6(Ω)δ and ujL6(Ω)=limnu+jnL6(Ω)δ>0. Similarly ujL6(Ω)δ>0,j=1,,k and we have U=(u1,,uk) is sign-changing.

    Proof of Theorem 1.1. First, obviously functions in XW are sign-changing. Given an integer l, by Proposition 2.1 the functional I(ε)p,0<ε1,2<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),pn3. 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)¯limnm(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 UlnU in X as ln. Then by Lemma 3.2, UlnU in X, DI(U)=0. Therefore

    +>m(U,I)¯limnm(Uln,I)limnln=+,

    we arrive at a contradiction.

    The work is supported by NSFC (11771324, 11831009, 11861021, 12071438).

    The authors declare there is no conflict of interest.



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