Existence of positive multi-bump solutions for a Schrödinger-Poisson system in R3 Claudianor O. Alvesa∗, Minbo Yangb† 5 1 a. Universidade Federal de Campina Grande 0 Unidade Acadêmica de Matemática 2 CEP: 58429-900,Campina Grande - Pb, Brazil n b. Department of Mathematics, Zhejiang Normal University a J Jinhua, 321004,P. R. China. 3 1 ] P Abstract A In this paper we are going to study a class of Schrödinger-Poissonsystem . h t −∆u+(λa(x)+1)u+φu=f(u) in R3, a m −∆φ=u2 in R3. (cid:26) [ Assuming that the nonnegative function a(x) has a potential well int(a−1({0})) 1 consisting of k disjoint components Ω1,Ω2,.....,Ωk and the nonlinearity f(t) has a v subcritical growth, we are able to establish the existence of positive multi-bump 0 solutions by variational methods. 3 9 Mathematics Subject Classifications (2010): 35J20, 35J65 2 0 . Keywords: Schrödinger-Poissonsystem, multi-bump solution, variational methods. 1 0 5 1 Introduction 1 : v This paper was motivated by some recent works concerning the nonlinear Schrödinger- i X Poisson system r a −i∂ψ = −∆ψ+V(x)ψ+φ(x)ψ−|ψ|p−2ψ in R3, ∂t (NSP) −∆φ= |ψ|2 in R3, (cid:26) whereV :R3 → Risanonnegativecontinuousfunctionwith inf V(x) >0,2 < p < 2∗ = 6 x∈R3 and ψ : Ω → C and φ: Ω→ R are two unknown functions. The first equation in system (NSP), called Schrödinger equation, describes quantum (non-relativistic) particles interacting with the eletromagnetic field generated by the motion. Aninteresting phenomenon ofthis Schrödinger type equation isthatthe potential ∗C. O. Alves was partially supported by CNPq/Brazil 301807/2013-2 and INCT-MAT, coalves@dme.ufcg.edu.br †M. Yang was supported by NSFC(11101374, 11271331), mbyang@zjnu.edu.cn 1 φ(x) is determined by the charge of wave function itself, that means, φ(x) satisfies the second equation (Poisson equation) in system (NSP). As we all know, the knowledge of the solutions for the elliptic system −∆u+V(x)u+φu = f(u) in R3, (SP) −∆φ= u2 in R3, (cid:26) has a great importance in studying stationary solutions ψ(x,t) = e−itu(x) of (NSP). It is convenient to observe that the system (SP) contains two kinds of nonlinearities. The first one is φ(x)u which is nonlocal, since the electrostatic potential φ(x) depends also on the wave function, and is used to describe the interaction between the solitary wave and the electric field. The second type of nonlinearity f(u) is a local one which has been used to model the external forces involving only functions of fields. For more information about the physical background of system (SP), we cite the papers of Benci-Fortunato [6], Bokanowski & Mauser [8], Mauser [24], Ruiz [26], Ambrosetti-Ruiz [4] and S’anchez & Soler [28]. Animportant factforsystem(SP)isthatitcanbereducedintoonesingleSchrödinger equation with a nonlocal term (see, for instance, [5, 17, 26, 30]). Effectively, by the Lax- Milgram Theorem, given u ∈ H1(R3), there exists an unique φ = φ ∈ D1,2(R3) such u that −∆φ= u2 in R3. Byusingstandardarguments, weknowthatφ verifiesthefollowing properties(foraproof u see [11, 26, 30]): Lemma 1.1. For any u ∈ H1(R3), we have u2(y) i) φ (x) = dy for all x ∈ R3; u R3 |x−y| Z ii) there exists C > 0 |∇φ |2dx = φ u2dx ≤ C||u||4 ∀u∈ H1(R3), u u H1(R3) R3 R3 Z Z 1 2 where ||u||H1(R3) = (|∇u|2+|u|2)dx . R3 (cid:18)Z (cid:19) iii) φ ≥ 0 ∀u∈ H1(R3); u iv) φ = t2φ , ∀t> 0 and u∈ H1(R3); tu u v) if u ⇀ u in H1(R3), then φ ⇀ φ in D1,2(R3) and n un u lim φ u2dx ≥ φ u2dx. n→+∞ R3 un n R3 u Z Z vi) if u → u in H1(R3), then φ → φ in D1,2(R3). Hence, n un u lim φ u2dx = φ u2dx. n→+∞ R3 un n R3 u Z Z 2 Therefore, (u,φ) ∈ H1(R3)×D1,2(R3) is a solution of (SP) if, and only if, u∈ H1(R3) is a solution of the nonlocal problem −∆u+V(x)u+φ u= f(u) in R3, u (P) u ∈H1(R3), (cid:26) where φ = φ∈ D1,2(R3). u Now, we would like to emphasize that the existence of solutions for problem (P) can be established via variational methods. Associated to the elliptic equation (P), we have the energy functional I : E → R given by 1 1 I(u) = ||u||2+ φ u2dx− F(u)dx, u 2 4 R3 R3 Z Z s where F(s) = f(t)dt and E is the function space 0 R E = u∈ H1(R3) : V(x)|u|2 < +∞ R3 (cid:26) Z (cid:27) endowed with the norm 1 2 kuk = (|∇u|2+V(x)|u|2)dx . R3 (cid:18)Z (cid:19) Supposingsomeconditionsonf,Lemma1.1impliesthatthefunctionalI iswelldefined and I ∈ C1(E,R) with I′(u)v = ∇u∇vdx+ V(x)uvdx+ φ uvdx− f(u)vdx ∀u,v ∈ E. u R3 R3 R3 R3 Z Z Z Z Hence, thecriticalpointsoffunctional I areinfacttheweak solutionsfornonlocalproblem (P). From the above commentaries, we know that the system (SP) has a nontrivial solution if, and only if, the nonlocal problem (P) has a nontrivial solution. In the last years, many authors had studied the system (SP) and focused their attentions to establish existence and nonexistence of solutions, multiplicity of solutions, ground state solutions, radial and nonradial solutions, semiclassical limit and concentrations of solutions, seefor example the papers of Azzollini & Pomponio [5], Cerami & Vaira [9], Coclite [10], D’Aprile & Mugnai [11, 12], d’Avenia [13], Ianni [19], Kikuchi [18], and Zhao & Zhao [30]. For the problem set in a bounded domain, we would like to cite the papers of Siciliano [17], Ruiz & Siciliano [27] and Pisani & Siciliano [25] for nonnegative solutions and Alves & Souto [3], Ianni [20] and Kim & Seok [22] for sign-changing solutions. However, related to the existence of multi-bump solutions for Schrödinger-Poisson system with potential well, as far as we know, there seems to be no existing results. In the present paper, we will assume that potential V(x) is of the form V(x)= λa(x)+1, 3 where λ is a positive parameter and a : R3 → R is a nonnegative continuous function. Hence, the problems (SP) and (P) can be written respectively as −∆u+(λa(x)+1)u+φu= f(u) in R3, (SP) −∆φ= u2 in R3, λ (cid:26) and −∆u+(λa(x)+1)u+φ u= f(u) in R3, u (P) u∈ H1(R3). λ (cid:26) To state the main result, we assume that the function a(x) verifying the following conditions: (a )Thesetint(a−1({0}))isnonemptyandtherearedisjointopencomponentsΩ ,Ω ,.....,Ω 1 1 2 k such that int(a−1({0})) = ∪k Ω (1.1) j=1 j and dist(Ω ,Ω ) > 0 for i 6= j, i,j = 1,2,··· ,k. (1.2) i j From (a ), we see that 1 a−1({0}) = ∪k Ω . (1.3) j=1 j Related to the function f, we will assume the ensuing conditions: f(s) (f ) lim = 0, 1 s→0 s f(s) (f ) lim = 0, 2 |s|→+∞ s5 (f ) There exists θ >4 such that 3 0< θF(s)≤ sf(s) ∀s∈ R\{0}. Moreover, we also assume that the nonlinearity f satisfies f(s) (f ) is increasing in |s|> 0. 4 s3 The motivation to investigate problem (SP) goes back to the papers [1] and [15]. In λ [15], inspired by [14] and [29], the authors considered the existence of positive multi-bump solution for the problem −∆u+(λa(x)+Z(x))u = uq in RN, (1.4) u∈ H1(RN), (cid:26) q ∈ (1, N+2) if N ≥ 3; q ∈(1,∞) if N = 1,2. The authors showed that the above problem N−2 has at least 2k −1 solutions u for large values of λ. More precisely, for each non-empty λ subset Υ of {1,...,k}, it was proved that, for any sequence λ → ∞ we can extract a n 4 subsequence (λ ) such that (u ) converges strongly in H1 RN to a function u, which ni λni satisfies u= 0 outside Ω = Ω and u , j ∈ Υ, is a least energy solution for Υ j∈Υ j |Ωj (cid:0) (cid:1) S −∆u+Z(x)u = uq, in Ω , j (1.5) (u∈ H01 Ωj , u > 0, in Ωj. (cid:0) (cid:1) After, in [1], Alves extended the results described above to the quasilinear Schrödinger equation driven by p-Laplacian operator. Involving the Schrödinger-Poisson system with potential wells, there are not so many existingpapers. Asfarasweknow,theonlypaperthatconsideredtheexistenceofsolutions forsystem(SP) isduetoJiangandZhou[21]wheretheauthorsstudiedtheexistenceand λ properties of the solutions depending on some parameters. However, nothing is known for the existence of multi-bump type solutions. Motivated by the above references, we intend in the present paper to study the existence of positive multi-bump solution for (SP) . λ However, we need to point out some difficulties involving this subject: 1-Itiswellknownthattheequation(1.5)playstheroleoflimitequationfor(1.4)asλgoes to infinity and the ground state solution of (1.5) plays an important role in building the multi-bump solutions for (1.4). However, little is known about what is the corresponding limit equation for equation (P) when the parameter λ goes to infinity. λ 2- Once discovered the limit problem for equation (P) , it is crucial to prove that it has λ a specially shaped least energy solution on a subset of the Nehari manifold , see Section 2 for more details. 3- When we apply variational methods to prove the existence of solution to (SP) , we are λ led to study a nonlocal, see problem (P) above. However, for this class of problem, it is λ necessary to make a careful revision in the sets used in the deformation lemma found in [1] and [15] to get multi-bump solution, since they don’t work well for this class of system, see Sections 6 and 7 for more details. Our main result is the following Theorem 1.2. Assume that (a ) and (f ) − (f ) hold. Then, there exist λ > 0 with 1 1 4 0 the following property: for any non-empty subset Υ of {1,2,...,k} and λ ≥ λ , problem 0 P has a positive solution u . Moreover, if we fix the subset Υ, then for any sequence λ λ λ → ∞ we can extract a subsequence (λ ) such that (u ) converges strongly in H1(R3) (cid:0)n (cid:1) ni λni to a function u, which satisfies u = 0 outside Ω = ∪ Ω , and u is a least energy Υ j∈Υ j |ΩΥ solution for the nonlocal problem u2(y) −∆u+u+ dy u= f(u) in Ω , Υ |x−y|  (cid:18)ZΩΥ (cid:19) (P)∞,Υ u(x) > 0 ∀x∈ Ω and ∀j ∈ Υ,  j  u∈ H1(Ω ). 0 Υ    5 In the proof of Theorem 1.2, we need to study the existence of least energy solution for problem (P) . The main idea is to prove that the energy function J associated with ∞,Υ nonlocal problem (P) given by ∞,Υ 1 1 J(u) = (|∇u|2 +|u|2)dx+ φ u2dx− F(u)dx, u 2 4 ZΩΥ ZΩΥ ZΩΥ assumes a minimum value on the set M = {u∈ N : J′(u)u = 0 and u 6= 0 ∀j ∈ Υ} Υ Υ j j where u = u and N is the corresponding Nehari manifold defined by j |Ωj Υ N = {u ∈ H1(Ω )\{0} : J′(u)u = 0}. Υ 0 Υ More precisely, we will prove that there is w ∈ M such that Υ J(w) = inf J(u). u∈MΥ After, we use a deformation lemma to prove that w is a critical point of J, and so, w is a least energy solution for (P) . The main feature of the least energy solution w is that ∞,Υ w(x) > 0 ∀x ∈ Ω and ∀j ∈ Υ which will be used to describe the existence of multi-bump j solutions. Since we intend to look for positive solutions, through this paper we assume that f(s)= 0, s ≤ 0. 2 The problem (P) ∞,Υ Inwhat follows, to show in details the idea of proving the existence of leastenergy solution for (P) , we will consider Υ = {1,2}. Moreover, we will denote by Ω, N and M the ∞,Υ sets Ω , N and M respectively. Thereby, Υ Υ Υ Ω = Ω ∪Ω , 1 2 N = {u ∈H1(Ω)\{0} : J′(u)u = 0} 0 and M = {u∈ N :J′(u)u = J′(u)u = 0 and u ,u 6= 0}, 1 2 1 2 with u = u , j = 1,2. j |Ωj Since we want to look for least energy for (P) , our goal is to prove the existence of ∞,Υ a critical point for J in the set M. 6 2.1 Technical lemmas In what follows, we will denote by || ||, || || and || || the norms in H1(Ω), H1(Ω ) and 1 2 0 0 1 H1(Ω ) given by 0 2 1 2 ||u|| = (|∇u|2+|u|2)dx , (cid:18)ZΩ (cid:19) 1 2 ||u|| = (|∇u|2+|u|2)dx 1 (cid:18)ZΩ1 (cid:19) and 1 2 ||u|| = (|∇u|2+|u|2)dx 2 (cid:18)ZΩ2 (cid:19) respectively. In order to show that the set M is not empty, we need of the following Lemma. Lemma 2.1. Let v ∈ H1(Ω) with v 6= 0 for j = 1,2. Then, there are t,s > 0 such that 0 j J′(tv +sv )v = 0 and J′(tv +sv )v = 0. 1 2 1 1 2 2 Proof. It what follows, we consider the vector field H(s,t)= J′(tv +sv )(tv ),J′(tv +sv )(sv ) . 1 2 1 1 2 2 (cid:0) (cid:1) From (f )−(f ), a straightforward computation yields that there are 0 < r < R such that 1 3 J′(rv +sv )(rv ), J′(tv +rv )(rv ) > 0, ∀s,t∈ [r,R] 1 2 1 1 2 2 and J′(Rv +sv )(Rv ), J′(tv +Rv )(Rv )< 0, ∀s,t∈ [r,R]. 1 2 1 1 2 2 Now, the lemma follows by applying Miranda theorem [23]. As an immediate consequence of the last lemma, we have the following corollary Corollary 2.2. The set M is not empty. Next, we will show some technical lemmas. Lemma 2.3. There exists ρ > 0 such that (i) J(u) ≥ ||u||2/4 and ||u|| ≥ ρ,∀u∈ N; (ii) ||w || ≥ ρ, ∀w ∈M and j = 1,2, where w = w| ,j = 1,2. j j j Ωj Proof. From (f ), for any u∈ N 4 4J(u) = 4J(u)−J′(u)u = ||u||2 + [uf(u)−4F(u)]dx ≥ ||u||2 ZΩ 7 and so, J(u) ≥ ||u||2/4, ∀u∈ N. From (f ) and (f ), there is C > 0 such that 1 2 λ f(s)s≤ 1s2+Cs6, for all s ∈R, 2 where λ is the first eigenvalue of (−∆,H1(Ω)). Since J′(u)u = 0, 1 0 λ ||u||2 < ||u||2+ φ u2dx = uf(u)dx ≤ 1 u2dx+C u6dx. u 2 ZΩ ZΩ ZΩ ZΩ Then, by Sobolev embeddings, 1 ||u||2 < ||u||2+Cˆ||u||6, 2 from where it follows that ||u|| ≥ ρ ∀u∈ N, 1 where ρ= 1 4, finishing the proof of (i). 2Cˆ If w ∈ M(cid:16) , (cid:17)we have that J′(w)w = J′(w)w = 0. Then, a simple computation gives 1 2 J′(w )w < 0 for j = 1,2, which implies j j ||w ||2 < ||w ||2+ φ (w )2dx < f(w )w dx, for j = 1,2. j j j j wj j j j ZΩj ZΩj As in (i), we can deduce that ||w || ≥ ρ for j = 1,2. j j Lemma 2.4. If (w ) is a bounded sequence in M and p ∈ (2,6), we have n liminf |w |pdx > 0 j = 1,2. n,j n ZΩj where w = w | for j = 1,2. n,j n Ωj Proof. From (f ) and (f ), given ε> 0 there exists C > 0 such that 1 2 f(s)s≤ ελ s2+C|s|p+εs6, for all s ∈ R. 1 Since w ∈ M, by Lemma 2.3 n ρ2 ≤ ||w ||2 < w f(w )dx ≤ ελ (w )2dx+C |w |pdx+ε (w )6dx n,j j n,j n,j 1 n,j n,j n,j ZΩj ZΩj ZΩj ZΩj that is, ρ2 ≤ ε λ (w )2dx+ (w )6dx +C |w |pdx. 1 n,j n,j n,j ZΩj ZΩj ! ZΩj 8 Using the boundedness of (w ), there is C such that n 1 ρ2 ≤ εC +C |w |pdx. 1 n,j ZΩj Fixing ε = ρ2 , we get 2C1 ρ2 |w |pdx ≥ , n,j 2C ZΩj showing that ρ2 liminf |w |pdx ≥ > 0. n,j n 2C ZΩj 2.2 Existence of least energy solution for (P) ∞,Υ In this subsection, our main goal is to prove the following result Theorem 2.5. Assume that (f )−(f ) hold. Then equation (P) possesses a positive 1 4 ∞,Υ least energy solution on the set M. Proof. In what follows, we denote by c the infimum of J on M, that is, 0 c = inf J(v). 0 v∈M From Lemma 2.3(i), we conclude that c > 0. 0 By Corollary 2.2, we know that M is not empty, then there is a sequence (w ) ⊂ M n satisfying limJ(w ) = c . n 0 n Still from Lemma 2.3(i), (w ) is a bounded sequence. Hence, without loss of generality, n we may suppose that there is w ∈H1(Ω) verifying 0 w ⇀ w in H1(Ω), n 0 w → w in Lp(Ω) ∀p∈ [1,2∗) n and w (x) → w(x) a.e. in Ω. n Then, (f ) combined with the compactness lemma of Strauss [7, Theorem A.I, p.338] gives 2 lim |w |pdx = |w |pdx, n,j j n ZΩj ZΩj lim w f(w )dx = w f(w )dx n,j n,j j j n ZΩj ZΩj 9 and lim F(w )dx = F(w )dx, n,j j n ZΩj ZΩj from where it follows together with Lemma 2.4 that w 6= 0 for j = 1,2. Then, by Lemma j 2.1 there are t,s > 0 verifying J′(tw +sw )w = 0 and J′(tw +sw )w = 0. 1 2 1 1 2 2 Next, we will show that t,s ≤ 1. Since J′(w )w = 0 for j = 1,2, n,j n,j ||w ||2 + φ (w )2dx+ φ (w )2dx = f(w )w dx n,1 1 wn,1 n,1 wn,2 n,1 n,1 n,1 ZΩ1 ZΩ1 ZΩ1 and ||w ||2+ φ (w )2dx+ φ (w )2dx = f(w )w dx. n,2 2 wn,2 n,2 wn,1 n,2 n,2 n,2 ZΩ2 ZΩ2 ZΩ2 Taking the limit in the above equalities, we obtain ||w ||2+ φ (w )2dx+ φ (w )2dx ≤ f(w )w dx 1 1 w1 1 w2 1 1 1 ZΩ1 ZΩ1 ZΩ and ||w ||2+ φ (w )2dx+ φ (w )2dx ≤ f(w )w dx. 2 2 w2 2 w1 2 2 2 ZΩ2 ZΩ2 ZΩ2 Recalling that J′(tw +sw )(tw )= J′(tw +sw )(sw )= 0, 1 2 1 1 2 2 it follows that t2||w ||2+t4 φ (w )2dx+t2s2 φ (w )2dx = f(tw )tw dx 1 2 w1 1 w2 1 1 1 ZΩ1 ZΩ1 ZΩ1 and s2||w ||2+s4 φ (w )2dx+t2s2 φ (w )2dx = f(sw )sw dx. 2 2 w2 2 w2 1 2 2 ZΩ2 ZΩ2 ZΩ2 Now, without loss of generality, we will suppose that s ≥ t. Under this condition, s2||w ||2 +s4 φ (w )2dx+s4 φ (w )2dx ≥ f(sw )sw dx 2 2 w2 2 w2 1 2 2 ZΩ2 ZΩ2 ZΩ2 and then 1 f(sw )sw f(w )w −1 ||w ||2 ≥ 2 2 − 2 2 (w )4dx. s2 2 2 (sw )4 (w )4 2 (cid:18) (cid:19) ZΩ2(cid:18) 2 2 (cid:19) If s> 1, the left side in this inequality is negative, but from (f ), the right side is positive, 4 thus we must have s ≤ 1, which also implies that t ≤ 1. Our next step is to show that J(tw +sw ) = c . Recalling that tw +sw ∈ M, we 1 2 0 1 2 derive that 1 c ≤ J(tw +sw ) = J(tw +sw )− J′(tw +sw )(tw +sw ). 0 1 2 1 2 1 2 1 2 4 10

Existence of positive multi-bump solutions for a Schr\"odinger-Poisson system in $\mathbb{R}^{3}$

Similar Existence of positive multi-bump solutions for a Schr\"odinger-Poisson system in $\mathbb{R}^{3}$