Open Access

Infinite solutions having a prescribed number of nodes for a Schrödinger problem

Boundary Value Problems20172017:135

https://doi.org/10.1186/s13661-017-0861-2

Received: 23 March 2017

Accepted: 10 August 2017

Published: 18 September 2017

Abstract

In this paper, we are concerned with the multiplicity of solutions for a Schrödinger problem. A weaker super-quadratic assumption is required for the nonlinearity. Then we give a new proof for the infinite solutions to the problem, having a prescribed number of nodes. It turns out that the weaker condition of the nonlinearity suffices to guarantee the infinitely many solutions. At the same time, a global characterization of the critical values of the non-radial nodal solutions are given.

Keywords

Schrödinger equationinfinite solutionsprescribed number of nodessuper-quadratic condition

1 Introduction

The semilinear equation
$$ -\Delta u+u=f(x,u),\quad u\in H^{1}\bigl(\mathbb{R}^{N}\bigr), $$
(1.1)
originates from various problems in physics and mathematical physics, and is called Euclidean field equation in cosmology [1], and nonlinear Klein-Gordon or Schrödinger equations when one is looking for certain types of solitary waves [2]. More generally, (1.1) can be explained as the case of \(p=2\) in a more general problem:
$$ -\Delta_{p} u+\vert u\vert ^{p-2}u=f(x,u),\quad u\in W^{1, p}\bigl(\mathbb{R} ^{N}\bigr). $$
(1.2)

Since (1.1) is invariant under rotations, it is natural to search for spherically symmetric solutions. The radial solutions of (1.1) are proved by Bartsch-Willem [3] and Liu-Wang [4]. The existence question of non-radial solutions to (1.1) or (1.2) was open for a long time [5], until it was proved by Bartsch-Willem [6] and Liu-Wang [4]. Fan [7] considered \(p(x)\)-Laplacian equations in \(\mathbb{R}^{N}\) with periodic data and nonperiodic perturbations being stationary at infinity, where the perturbations are carried out not only on the coefficients but also on the exponents. Using the concentration-compactness principle, Fan proved the existence of ground state solutions vanishing at infinity under appropriate assumptions. Later Alves-Liu [8] improved the result of Fan in [7], and obtained ground states of \(p(x)\)-Laplacian equations in \(\mathbb{R}^{N}\). They also established a Bartsch-Wang type compact embedding theorem for variable exponent spaces. Ayoujil [9] was concerned with the existence and multiplicity of solutions to the \(p(x)\)-Laplacian Steklov problem without the well-known Ambrosetti-Rabinowitz type growth conditions. By means of critical point theorems with Cerami condition, he proved the existence and multiplicity results of the solutions under weaker conditions.

For the equation
$$ -\Delta_{p} u=f(x,u),\quad u\in W^{1, p}_{0}(\Omega), $$
(1.3)
where Ω is a bounded domain in \(\mathbb{R}^{N}\), Dinca-Jebelean-Mawhin [10] obtained the existence results under Dirichlet boundary condition. Bartsch-Liu [11] proved the existence of several solutions of (1.3), that is, a pair of subsolution and supersolution, a positive and a negative solution, and a sign-changing solution. Bonanno-Candito [12] established the existence of three solutions for the Neumann boundary condition of (1.3).
In this paper, we are concerned with the multiple solutions of (1.2), and require the following assumptions on the nonlinearity \(f(x, u)\):
\((f_{1})\)

\(f(x, 0)=0\), \(f(x, t)=o(\vert t\vert ^{p-2}t)\), as \(\vert t\vert \rightarrow 0\), uniformly in x.

\((f_{2})\)
\(f\in C(\mathbb{R}^{N}, \mathbb{R})\) and there exist \(C>0\) and \(q\in (p, p^{*})\) such that
$$\bigl\vert f(x, t)\bigr\vert \leq C\bigl(1+\vert t\vert ^{q-1} \bigr), $$
where \(p^{*}=Np/(N-p)\) if \(N>p\), and \(p^{*}=\infty \) if \(N\leq p\).
\((f_{3})\)

\(\lim_{\vert t\vert \rightarrow \infty }\frac{F(x, t)}{\vert t\vert ^{p}}=+\infty \), where \(F(x, t)= \int^{t}_{0}f(x, s)\,ds\).

\((f_{4})\)

There exists \(R>0\) such that, for any x, \(\frac{f(x, t)}{\vert t\vert ^{p-2}t}\) is increasing in \(t\geq R\), and decreasing in \(t\leq -R\).

Remark 1.1

The assumption \((f_{3})\) comes from the following condition:
$$\lim_{\vert t\vert \rightarrow \infty }\frac{f(x, t)}{\vert t\vert ^{p-2}t}=+\infty. $$
In the case \(p=2\), \((f_{3})\) characterizes problem (1.2) as superlinear at infinity. It is an extension of a very natural super-quadratic condition (SQ condition for short), SQ condition: \(\lim_{\vert t\vert \rightarrow \infty }\frac{F(x, t)}{t^{2}}=\infty\).

Remark 1.2

The SQ condition is weaker than the famous Ambrosetti-Rabinowitz growth condition (AR condition for short). Since the work of Ambrosetti-Rabinowitz [13], the AR condition has most frequently appeared in the superlinear elliptic boundary value problem. AR condition: There exist \(\mu >p\) and \(R>0\) such that
$$0< \mu F(x, t)\leq f(x, t) t,\quad \mbox{for } x\in D \mbox{ and } \vert t\vert \geq R. $$
It is important not only in establishing the mountain-pass geometry of the functional, but also in obtaining the bounds of PS sequences. In fact, the AR condition implies that, for some \(C>0\),
$$F(x, t)\geq C\vert t\vert ^{\mu },\quad \mu >p. $$

In recent years there were some articles trying to drop the AR condition in the study of the superlinear problems. For equation (1.1), Liu-Wang [4] first posed the SQ condition to get the bounds of a minimizing sequence on the Nehari manifold. Furthermore, under coercive conditions of a potential function \(V(x)\), they proved the existence of three solutions of equation \(-\Delta u+V(x)u=f(x,u)\) (\(u\in H^{1}(\mathbb{R}^{N})\)), one positive, one negative and one sign-changing solution. Later Li-Wang-Zeng [14] gave a natural generalization of Liu-Wang’s results [4] to two noncompact cases, which do not have compact embedding. We made use of a combination of the techniques in [4] and the concentration-compactness principle of Lions [15, 16]. Then we gave general conditions which ensure the existence of ground state solutions. Miyagaki-Souto [17] established the existence of a nontrivial solution of (1.1) by combining some arguments of Struwe-Tarantello in [18]. Then Liu [19] extended the results of Miyagaki-Souto [17], and obtained the existence and multiplicity results for superlinear p-Laplacian equations (1.2) without the AR condition. To overcome the difficulty that the Palais-Smale sequences of the Euler-Lagrange functional may be unbounded, they consider the Cerami sequences.

Tan-Fang [20] considered the \(p(x)\)-Laplacian equations on the bounded domain and expanded a recent result [21] of Gasinski-Papageorgiou. The nonlinearity is superlinear but does not satisfy the usual AR condition near infinity, or its dual version near zero. They obtained the existence and multiplicity results via Morse theory and modified functional methods. Ge [22] dealt with the superlinear elliptic problem without Ambrosetti-Rabinowitz type growth condition in a bounded domain with smooth boundaries. He obtained the existence results of nontrivial solutions for every parameter. Using variational arguments, Carvalho-Goncalves-Silva [23] established the existence of multiple solutions for quasilinear elliptic problems driven by the Φ-Laplacian operator.

The main result of this paper is as follows.

Theorem 1.3

Under the assumptions \((f_{1})\)-\((f_{4})\), for every integer \(k>0\), there exist a pair \(u^{+}_{k}\) and \(u_{k}^{-}\) of radial solutions of (1.2) with \(u_{k}^{-}(0)<0<u_{k}^{+}(0)\), having exactly k nodes; \(0<\rho_{1}^{\pm }<\cdots <\rho_{k}^{\pm }<\infty \).

Here a node \(\rho >0\) is defined such that \(u(\rho)=0\).

Theorem 1.4

Under the assumptions \((f_{1})\)-\((f_{4})\) and if \(f(x, u)\) is odd in u, there exist infinitely many non-radial nodal solutions of (1.2).

Remark 1.5

It is also possible to replace the oddness of \(f(x, u)\) in Theorem 1.4 by other conditions, we refer the reader to the work of Jones-Küpper [24].

We further assume that:
\((f_{5})\)
\(f\in C(\mathbb{R}^{N}, \mathbb{R})\) and for some \(C>0\),
$$\bigl\vert f'_{u}(x, t)\bigr\vert \leq C\bigl(1+ \vert t\vert ^{q-2}\bigr), $$
where \(q=p^{*}\) if \(N\geq 3\) and \(q\in (p, p^{*})\) if \(N=2\).

Corollary 1.6

Assume \(N=4\) or \(N\geq 6\), the assumptions \((f_{2})\)-\((f_{5})\) hold, and f is odd in u. Then equation (1.2) has an unbounded sequence of non-radial sign-changing solutions.

In the present paper, we give a new proof for the infinite solutions to problem (1.2) having a prescribed number of nodes, and the results are proved under the weaker SQ condition. It turns out that the SQ condition on \(f(x, u)\) suffice to guarantee infinitely many solutions. Our theorems generalize the results in [4] to the case of \(p\neq 2\). At the same time, a global characterization of the critical values of the nodal radial solutions are given.

2 Preliminaries

In this section, we give some notations and some preliminary lemmas, which will be adopted in Section 3.

Solutions of (1.2) correspond to the critical points of the functional
$$J(u):= \int_{\mathbb{R}^{N}}\frac{1}{p}\vert \nabla u\vert ^{p}+\frac{1}{p}\vert u\vert ^{p}-F(x,u),\quad u\in W^{1,p}\bigl(\mathbb{R}^{N}\bigr), $$
where \(W^{1,p}(\mathbb{R}^{N})\) is endowed with the norm \(\Vert u\Vert = (\int_{\mathbb{R}^{N}}(\vert \nabla u\vert ^{p}+\vert u\vert ^{p}))^{\frac{1}{p}}\).

Notation 2.1

We define the Nehari manifold
$$\mathcal{N}_{1}=\bigl\{ u\in X_{1}: u\neq 0, \bigl\langle J'(u), u\bigr\rangle =0\bigr\} , $$
where \(X_{1}:=\{u\in W^{1,p}(\mathbb{R}^{N}):u(x)=u(\vert x\vert )\}\). And
$$\mathcal{N}_{2}=\bigl\{ u\in X_{2}: u\neq 0, \bigl\langle J'(u), u\bigr\rangle =0\bigr\} , $$
where \(X_{2}:=W^{1,p}(\mathbb{R}^{N})\). For \(0\leq \rho <\sigma \leq \infty \), we define
$$\begin{aligned}& \Omega (\rho, \sigma):= \operatorname{int}\bigl\{ x\in \mathbb{R}^{N}: \rho \leq \vert x \vert \leq \sigma \bigr\} , \\& X_{\rho, \sigma }:=\bigl\{ u\in W^{1,p}\bigl(\Omega (\rho, \sigma) \bigr):u(x)=u\bigl(\vert x\vert \bigr) \bigr\} , \\& \mathcal{N}_{\rho, \sigma }=\bigl\{ u\in X_{\rho, \sigma }: u\neq 0, \bigl\langle J'(u), u\bigr\rangle =0\bigr\} . \end{aligned}$$
Define \(u(x)=0\) for \(x \notin \Omega (\rho, \sigma)\) if \(u\in X_{1}\). Obviously \(X_{\rho, \sigma }\subset X_{1}\) and \(\mathcal{N}_{\rho, \sigma }\subset \mathcal{N}_{1}\).
We fix k, and we define
$$\begin{aligned} \mathcal{N}^{+}_{k} =&\bigl\{ u\in X_{1}: \mbox{there exist } 0=\rho_{0}< \rho_{1}< \cdots < \rho_{k}< \rho_{k+1}=\infty , \mbox{such that } \\ &{}(-1)^{j}u\vert _{\Omega (\rho_{j}, \rho_{j+1})}\geq 0 \mbox{ and } u\vert _{ \Omega (\rho_{j}, \rho_{j+1})}\in \mathcal{N}_{\rho_{j}, \rho_{j+1}}, \mbox{for } j=0, \ldots,k \bigr\} . \end{aligned}$$
On \([0, \infty)\times \mathbb{R}\), we define
$$f^{+}(r, u)=\textstyle\begin{cases} f(r, u), & \mbox{if } u\geq 0, \\ -f(r, -u),& \mbox{if } u< 0, \end{cases} $$
and \(F^{+}(r, u):= \int_{0}^{u}f^{+}(r, s)\,ds\),
$$J^{+}(u):= \int_{\mathbb{R}^{N}}\frac{1}{p}\vert \nabla u\vert ^{p}+\frac{1}{p}\vert u\vert ^{p}-F ^{+}(x,u). $$
Similarly, we define
$$f^{-}(r, u)=\textstyle\begin{cases} f(r, u), & \mbox{if } u\leq 0, \\ -f(r, -u), & \mbox{if } u>0, \end{cases} $$
and \(F^{-}(r, u)\), \(J^{-}(u)\).

The letters C will always denote various universal constants.

Lemma 2.2

Under assumptions \((f_{1})\)-\((f_{4})\), the equation
$$ -\Delta_{p} u+\vert u\vert ^{p-2}u=f(x,u),\quad u\in X_{\rho, \sigma } , $$
(2.1)
has a weak solution u such that
$$J(u)=\max_{t>0}J(tu)=\inf_{v\in X_{\rho, \sigma }\backslash \{0\}} \max _{t>0}J(tv)>0. $$

Proof

By the assumptions \((f_{1})\) and \((f_{2})\), J has a strict local minimum at 0. For any \(u\neq 0\), \(J(tu)\rightarrow - \infty \) as \(t\rightarrow \infty \). Thus
$$ c:=\inf_{v\in X_{\rho, \sigma }\backslash \{0\}}\max_{t>0} J(tv)>J(0)=0 $$
(2.2)
is well defined.
Let \(\{u_{n}\}\) be a minimizing sequence of c such that
$$J(u_{n})=\max_{t>0} J(tu_{n})\rightarrow c $$
as \(n\rightarrow \infty \).

First we want to prove that \(\{u_{n}\}\) is bounded. If not, consider \(v_{n}:=u_{n}/\Vert u_{n}\Vert \), then \(\Vert v_{n}\Vert =1\). By passing to a subsequence, we may assume \(v_{n}\rightarrow v\) weakly in \(X_{\rho, \sigma }\) and strongly in \(L^{r}(X_{\rho, \sigma })\) for any \(r\in [p, p^{*}]\). Note that \((f_{1})\) and \((f_{2})\) imply \(\int_{X_{\rho, \sigma }}F(x, u)\) is weakly continuous on \(X_{\rho, \sigma }\).

If \(v\neq 0\), we have
$$\frac{c+o(1)}{\Vert u_{n}\Vert ^{p}}=\frac{1}{p}- \int_{X_{\rho, \sigma }}\frac{F(x, u_{n})}{u_{n}^{p}}v_{n}^{p}. $$
By (2.2),
$$\frac{1}{p}> \int_{X_{\rho, \sigma }}\frac{F(x, u_{n})}{u_{n}^{p}}v _{n}^{p}. $$
Then by \((f_{3})\) and Fadou’s lemma, passing to the limit on both sides,
$$\frac{1}{p}> \int_{X_{\rho, \sigma }}\frac{F(x, u_{n}(x))}{u_{n}^{p}}v ^{p}=\infty. $$
This gives a contradiction.
If \(v=0\), fixing an \(R>\sqrt[p]{pc}\), by \(\Vert v_{n}\Vert =1\), we have
$$J(u_{n})\geq J(Rv_{n})=\frac{1}{p}R^{p}- \int_{X_{\rho, \sigma }}F(x, Rv_{n}). $$
\(J(u_{n})\) converges towards c, but \(R^{p}/p-\int_{X_{\rho, \sigma }}F(x, Rv_{n})\) tends to \(R^{p}/p>c\), a contradiction. Thus \(\{u_{n}\}\) is bounded.
Assume \(u_{n}\) weakly converges to u. As \(n\rightarrow \infty \),
$$\int_{X_{\rho, \sigma }}u_{n}f(x, u_{n})\rightarrow \int_{X_{\rho, \sigma }}uf(x, u). $$
Since, for some \(\alpha >0\), \(\Vert u_{n}\Vert ^{p}>\alpha \), and
$$\Vert u_{n}\Vert ^{p}= \int_{X_{\rho, \sigma }}u_{n}f(x, u_{n}), $$
so \(u\neq 0\).
There is \(s>0\) such that \(J(su)= \max_{t>0} J(tu)\). Then
$$J(su)\leq \liminf_{n\rightarrow \infty } J(su_{n})\leq \liminf _{n\rightarrow \infty } J(u_{n})=c. $$

\((f_{4})\) implies that \(\max_{t>0} J(tu)\) is achieved at only one point \(t=s\). It is also the unique one such that \(\langle J'(tu), u\rangle =0\).

Next we claim that su is a critical point of J. Without loss of generality, we assume \(s=1\). If u is not a critical point, there is \(v\in C_{0}^{\infty }(\Omega)\) such that \(\langle J'(u), v\rangle =-2\). There is \(\varepsilon_{0}>0\) such that, for \(\vert t-1\vert +\vert \varepsilon \vert \leq \varepsilon_{0}\), \(\langle J'(tu+\varepsilon v)\), \(v\rangle \leq -1\).

If \(\varepsilon >0\) is small, let \(t_{\varepsilon }>0\) be the unique number such that
$$\max J(tu+sv)= J(t_{\varepsilon }u+\varepsilon v). $$
Then \(t_{\varepsilon }\rightarrow 1\) as \(\varepsilon \rightarrow 0\).
If ε is small such that \(\vert t_{\varepsilon }-1\vert +\varepsilon \leq \varepsilon_{0}\), then \(J(t_{\varepsilon }u+\varepsilon v) \geq c\), but by the assumption that \(\langle J'(tu+\varepsilon v)\), \(v\rangle \leq -1\), so
$$J(t_{\varepsilon }u+\varepsilon v)= J(t_{\varepsilon }u)+ \int^{1}_{0} \bigl\langle J'(t_{\varepsilon }u+s \varepsilon v), \varepsilon v\bigr\rangle \,ds \leq c-\varepsilon < c. $$
This is a contradiction. □

Lemma 2.3

Under assumptions \((f_{2})\)-\((f_{5})\), if f is odd in u, equation (2.1) has infinitely many pairs of solutions.

Proof

It is clear that the solutions occur in pairs due to the oddness of \(f(x, u)\). Under the assumptions, any critical point of J restricted on \(\mathcal{N}_{2}\) is a critical point of J in \(X_{2}\). To verify the PS condition it suffices to show that any PS sequence is bounded. This is similar to the proof of Lemma 2.2. We omit the details.

If the PS condition is satisfied on \(\mathcal{N}_{2}\), then the standard Ljusternik-Schnirelmann theory gives rise to an unbounded sequence of critical values of J; see the details in [25]. □

3 Proof of theorems

In this section, we prove Theorem 1.3 and Theorem 1.4.

Proof of Theorem 1.3

First by Lemma 2.2, the infimum
$$c^{+}(\rho, \sigma):=\inf_{\mathcal{N}_{\rho, \sigma }}J^{+} $$
is achieved. Since \(\vert u\vert \) is also a minimizer, we assume the minimizer u is a positive solution of the problem
$$ -\Delta_{p} u+\vert u\vert ^{p-2}u=f(x,u),\quad u\in X_{\rho, \sigma }. $$
(3.1)
Similarly, the infimum
$$c^{-}(\rho, \sigma):=\inf_{\mathcal{N}_{\rho, \sigma }}J^{-} $$
is also achieved by negative minimizers which are negative solutions of (3.1).
Then we work on the Nehari manifold \(\mathcal{N}_{k}^{+}\), and construct a \(u^{+}_{k}\in \mathcal{N}^{+}_{k}\) such that
$$c^{+}_{k}:=\inf_{\mathcal{N}^{+}_{k}}J $$
is achieved by some \(u^{+}_{k}\), which gives the desired solutions in Theorem 1.3.

Let \(\{u_{n}\}\) be a minimizing sequence of \(c^{+}_{k}\). As the same arguments hold in the proof of Lemma 2.2, \(\{u_{n}\}\) is bounded.

Since \(u_{n}\in \mathcal{N}^{+}_{k}\), there exist \(0=\rho_{0}^{n}<\rho _{1}^{n}<\cdots <\rho_{k}^{n}<\rho^{n}_{k+1}=\infty \) such that \((-1)^{j}u_{n}\vert _{\Omega (\rho_{j}^{n}, \rho_{j+1}^{n})}\geq 0\) and \(u_{n}\vert _{\Omega (\rho_{j}^{n}, \rho_{j+1}^{n})}\in \mathcal{N}_{\rho_{j}^{n}, \rho_{j+1}^{n}}\) for \(j=0, \ldots,k\).

Note that
$$\Vert u_{n}\vert _{\Omega (\rho_{j}^{n}, \rho_{j+1}^{n})}\Vert ^{p}= \int_{\Omega (\rho_{j}^{n}, \rho_{j+1}^{n})}u_{n}f(r, u_{n}). $$
By \((f_{1})\)-\((f_{2})\), 0 is a strict local minimizer of J, thus there is a \(\delta >0\) such that \(\Vert u\Vert \geq \delta \) for \(u\in \mathcal{N} _{\rho_{j}^{n}, \rho_{j+1}^{n}}\). Fix \(q\in (p, p^{*})\), and for any \(\varepsilon >0\), there is a constant \(C>0\) such that
$$\int_{\Omega (\rho_{j}^{n}, \rho_{j+1}^{n})}u_{n}f(r, u_{n})\leq \varepsilon \int_{\Omega (\rho_{j}^{n}, \rho_{j+1}^{n})}\vert u_{n}\vert ^{p}+C \int_{\Omega (\rho_{j}^{n}, \rho_{j+1}^{n})}\vert u_{n}\vert ^{q}, $$
where \(q\in (p, p^{*})\). Therefore, by choosing \(\varepsilon >0\) small we find a \(C>0\) such that
$$ \delta^{p}\leq \Vert u_{n}\vert _{\Omega (\rho_{j}^{n}, \rho_{j+1}^{n})}\Vert ^{p} \leq C \int_{\Omega (\rho_{j}^{n}, \rho_{j+1}^{n})}\vert u_{n}\vert ^{q}. $$
(3.2)
Using (3.2), in a similar way as in [3], we see that \(\{\rho_{k+1}^{n}\}_{n}\) is bounded away from ∞, \(\{\rho_{j+1} ^{n}-\rho_{j}^{n}\}_{n}\) is bounded away from 0 for each j, and there are \(0=\rho_{0}<\rho_{1}<\cdots <\rho_{k}<\rho_{k+1}=\infty \) such that \(\rho_{j}^{n}\rightarrow \rho_{j}\) as \(n\rightarrow \infty \), for \(j=1, \ldots, k\).

Along a subsequence of \(\{u_{n}\}\), we may assume that \(u_{n}\rightarrow u\) weakly in \(X_{1}\), and strongly in \(L^{r}(X_{1})\) for any \(r\in [p, p^{*}]\). It follows that \(u_{n}\vert _{\Omega (\rho_{j}^{n}, \rho_{j+1}^{n})}\rightarrow u\vert _{\Omega (\rho_{j}, \rho_{j+1})}\) weakly in \(X_{1}\), and strongly in \(L^{r}(X_{1})\) (\(r\in [p, p^{*})\)). And \((-1)^{j}u\vert _{\Omega (\rho_{j}, \rho_{j+1})}\geq 0\), for \(u\in \mathcal{N}_{\rho_{j}^{n}, \rho_{j+1}^{n}}\).

Let \(n\rightarrow \infty \) in (3.2). It implies that \(u\vert _{\Omega (\rho _{j}, \rho_{j+1})}\neq 0\). Thus we can choose an \(\alpha_{j}>0\) such that \(\alpha_{j}u\vert _{\Omega (\rho_{j}, \rho_{j+1})}\in \mathcal{N}_{( \rho_{j}, \rho_{j+1})}\) for \(j=1, \ldots, k\). Define
$$u_{k}^{+}:=\sum^{k}_{j=0} \alpha_{j}u\vert _{\Omega (\rho_{j}, \rho_{j+1})}. $$
By the definition of \(u_{k}^{+}\), we observe that \(u_{k}^{+}\in \mathcal{N}_{k}^{+}\).
Next we want to show
  1. 1.

    \(c_{k}^{+}\) is archived by \(u_{k}^{+}\), that is, \(J(u_{k}^{+})=c_{k} ^{+}\),

     
  2. 2.

    \(u_{k}^{+}\) is a radial function having nodes \(0<\rho_{1}<\cdots <\rho _{k}<\infty \),

     
  3. 3.

    \(u_{k}^{+}\) is a solution of (1.2).

     
The weak convergence of \(u_{n}\vert _{\Omega_{(\rho_{j}^{n}, \rho^{n}_{j+1})}}\) in \(X_{1}\) and strong convergence in \(L^{r}(X_{1})\) (\(p< r< p ^{*}\)) imply
$$ c_{k}^{+}\leq J\bigl(u_{k}^{+} \bigr)=\sum_{j=0}^{k} J( \alpha_{j}u\vert _{\Omega (\rho _{j},\rho_{j+1})})\leq \sum _{j=0}^{k}\liminf_{n\rightarrow \infty } J( \alpha_{j}u_{n}\vert _{\Omega (\rho_{j}^{n}, \rho^{n}_{j+1})}). $$
(3.3)
Also
$$ \sum_{j=0}^{k}\liminf_{n\rightarrow \infty } J(u_{n}\vert _{\Omega (\rho _{j}^{n}, \rho^{n}_{j+1})})= \liminf_{n\rightarrow \infty } J(u_{n})=c _{k}^{+}. $$
(3.4)
So \(J(u_{k}^{+})=c_{k}^{+}\).
Then the equality in (3.3) implies that \(\alpha_{j}u\vert _{\Omega (\rho_{j}^{n}, \rho^{n}_{j+1})}\) is a minimizer of
$$\inf_{\mathcal{N}_{\rho_{j}^{n}, \rho^{n}_{j+1}}\cap P^{+}} J^{+},\quad \mbox{if } j \mbox{ is even}, $$
and a minimizer of
$$\inf_{\mathcal{N}_{\rho_{j}^{n}, \rho^{n}_{j+1}}\cap P^{-}} J^{-},\quad \mbox{if } j \mbox{ is odd}, $$
where \(P^{\pm }:=\{u\in X_{1}:\pm u\geq 0\}\). At the same time, \(\alpha_{j}u\vert _{\Omega (\rho_{j}, \rho_{j+1})}\) is a minimizer of \(\inf_{\mathcal{N}_{\rho_{j}, \rho_{j+1}}} J^{\pm }\). When j is even, \(\alpha_{j}u\vert _{\Omega (\rho_{j}^{n}, \rho^{n}_{j+1})}\) is a positive solution of (1.2), and when j is odd, \(\alpha_{j}u\vert _{\Omega (\rho _{j}^{n}, \rho^{n}_{j+1})}\) is a negative solution. Then the strong maximum principle implies that \(u_{k}^{+}(0)>0\) and \((-1)^{j}u_{k} ^{+}(x)>0\), for \(\rho_{j}<\vert x\vert <\rho_{j+1}\) (\(j=0, 1, \ldots, k\)), and
$$(-1)^{j}\lim_{\vert x\vert \uparrow \rho_{j}}\frac{\partial u_{k}^{+}(x)}{ \partial \vert x\vert }>0,\qquad (-1)^{j}\lim_{\vert x\vert \downarrow \rho_{j}}\frac{\partial u_{k}^{+}(x)}{\partial \vert x\vert }>0,\quad \mbox{for } j=1, \ldots, k. $$
So \(u_{k}^{+}\) has exactly k nodes.
In order to prove \(u_{k}^{+}\) is a solution of (1.2), for simplicity we assume \(\alpha_{j}=1\) for all j. If \(u_{k}^{+}\) is not a critical point of J, then there is a \(\varphi \in C_{0}^{\infty }(\mathbb{R}^{N})\) such that
$$\bigl\langle J'\bigl(u_{k}^{+}\bigr), \varphi \bigr\rangle =-2. $$
Observe that there is a \(\tau >0\) such that, if \(\vert s_{j}-1\vert \leq \tau \) (\(j=0, \ldots, k\)) and \(0\leq \varepsilon \leq \tau \), the function
$$g(s, \varepsilon):= \sum_{j=0}^{k}s_{j}u \vert _{\Omega (\rho_{j}, \rho_{j+1})}+\varepsilon \varphi, $$
where \(s=(s_{1}, \ldots, s_{k})\), has exactly k nodes \(0<\rho_{1}(s, \varepsilon)<\cdots <\rho_{k}(s, \varepsilon)<\infty\). And \(\rho_{j}(s, \varepsilon)\) is continuous in \((s, \varepsilon)\in D \times [0, \tau ]\), where \(D:=\{(s_{1}, \ldots, s_{k})\in \mathbb{R}^{k}:\vert s _{j}-1\vert \leq \tau \}\), and
$$ \bigl\langle J'\bigl(g(s, \varepsilon)\bigr), \varphi \bigr\rangle < -1. $$
(3.5)
In order to deduce a contradiction, we set \(s\in D\), and
$$g_{1}(s)=\sum_{i=0}^{k}s_{i}u \vert _{\Omega (\rho_{i}, \rho_{i+1})}+\tau \eta (s) \varphi, $$
where \(\eta (s): D\rightarrow [0, 1]\) (\(s=(s_{1}, \ldots, s_{k})\)) is a cut-off function such that
$$\eta (s_{1}, \ldots, s_{k})=\textstyle\begin{cases} 1, & \mbox{if } \vert s_{i}-1\vert \leq \tau /4 \mbox{ for all } i, \\ 0, & \mbox{if } \vert s_{i}-1\vert \geq \tau /2 \mbox{ for at least one } i. \end{cases} $$
Then, for each \(s\in D\), \(g_{1}(s)\in C(D, X)\) and \(g_{1}(s)\) has exactly k nodes \(0<\rho_{1}(s)<\cdots <\rho_{k}(s)<\infty \), where \(\rho_{j}(s)\) is continuous.
Further, we define for \(j=1, \ldots, k\),
$$h_{j}(s):= \bigl\langle J'\bigl(g_{1}(s) \bigr) \vert _{\Omega (\rho_{j}(s), \rho_{j+1}(s))}, g_{1}(s) \vert _{\Omega (\rho_{j}(s), \rho_{j+1}(s))} \bigr\rangle . $$
And we define \(h: D\rightarrow \mathbb{R}^{k}\) as \(h(s):=(h_{1}(s), \ldots, h_{k}(s))\). Then \(h(s)\in C(D, \mathbb{R}^{k})\).
For a fixed j, if \(\vert s_{j}-1\vert =\tau \) then \(\eta (s)=0\) and \(\rho_{i}(s)=\rho_{i}\) for all \(i=1, \ldots, k\). So by the definition of \(g_{1}(s)\),
$$h_{j}(s)=\bigl\langle J'(s_{j}u)\vert _{\Omega (\rho_{j}, \rho_{j+1})}, s_{j}u\vert _{ \Omega (\rho_{j}, \rho_{j+1})}\bigr\rangle = \textstyle\begin{cases} >0, & \mbox{if } s_{j}=1-\tau, \\ < 0,& \mbox{if } s_{j}=1+\tau. \end{cases} $$
Therefore, the degree \(\operatorname{deg}(h, \operatorname{int}(D), 0)\) is well defined and \(\operatorname{deg}(h, \operatorname{int}(D), 0)=(-1)^{k}\). Thus there is an \(s\in \operatorname{int}(D)\) such that \(h(s)=0\), that is, \(g_{1}(s)\in \mathcal{N}_{k}^{+}\).
It is obvious that
$$ J\bigl(g_{1}(s)\bigr)\geq c_{k}^{+}. $$
(3.6)
On the other hand, by (3.5),
$$\begin{aligned} J\bigl(g_{1}(s)\bigr) =& J\Biggl(\sum_{j=0}^{k}s_{j}u \vert _{\Omega (\rho_{j}, \rho_{j+1})}\Biggr)+ \int^{1}_{0} \Biggl\langle J'\Biggl( \sum_{j=0}^{k}s_{j}u\vert _{\Omega (\rho_{j}, \rho_{j+1})}+\theta \tau \eta (s) \varphi \Biggr), \tau \eta (s) \varphi \Biggr\rangle \,d\theta \\ \leq& J\Biggl(\sum_{j=0}^{k}s_{j}u \vert _{\Omega (\rho_{j}, \rho_{j+1})}\Biggr)-\tau \eta (s). \end{aligned}$$
If \(\vert s_{j}-1\vert \leq \tau /2\) for each j, then by (3.4)
$$ J\bigl(g_{1}(s)\bigr)< J\Biggl(\sum_{j=0}^{k}s_{j}u \vert _{\Omega (\rho_{j}, \rho_{j+1})}\Biggr) \leq \sum_{j=0}^{k} J(u\vert _{\Omega (\rho_{j}, \rho_{j+1})})=c_{k}^{+}, $$
(3.7)
which contradicts (3.6).
If \(\vert s_{j}-1\vert >\tau /2\) for at least one j, by (3.4)
$$ J\bigl(g_{1}(s)\bigr)\leq J\Biggl(\sum_{j=0}^{k}s_{j}u \vert _{\Omega (\rho_{j}, \rho_{j+1})}\Biggr)< \sum_{j=0}^{k} J(u\vert _{\Omega (\rho_{j}, \rho_{j+1})})=c_{k}^{+}, $$
(3.8)
which is a contradiction with (3.6) too. The proof is finished. □

Proof of Theorem 1.4

Using a result of Lions in [26], it is possible to find a subspace E of \(X_{2}\) consisting of functions which are not radial and such that the inclusion \(E\hookrightarrow L^{s}\) is compact for \(p< s< p^{*}\); see the details in Theorem IV.1 of [26] or the proof of Theorem 2.1 in [6]. By Proposition 3.2 in [6], the subspace E should be chosen to satisfy the compactness. Here we describe E briefly. Let G be a group acting on \(X_{2}\) via orthogonal maps \(\varrho (g):X_{2}\rightarrow X_{2}\), such that the functional J is G-invariant, and the inclusion \(X_{2}^{G}\hookrightarrow L^{s}\) is compact for \(p< s< p^{*}\), where \(X_{2}^{G}:=\{u\in X_{2}, \varrho (g)u=u,\mbox{ for all }g\in G\}\). We set \(E:=X_{2}^{G}\). Then we follow the same steps in Lemma 2.2, and combine with Lemma 2.3 to get the infinitely many non-radial nodal solutions of (1.2). □

4 Conclusion

We are concerned with the multiplicity of solutions for a Schrödinger problem. Based on our work [14] about (1.1), which gave a natural generalization of Liu-Wang’s results [4] to two noncompact cases, we give a new proof for the infinite solutions having a prescribed number of nodes to problem (1.2) in the present paper. It turns out that the weaker condition of the nonlinearity suffices to guarantee the infinitely many solutions.

Declarations

Acknowledgements

The author is supported by the National Natural Science Foundation of China (NSFC, 11501110). She thanks the anonymous referee for a careful and thorough reading of the manuscript.

Open Access This article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.

Authors’ Affiliations

(1)
School of Mathematics and Computer Sciences, Fujian Normal University

References

  1. Coleman, S, Glazer, V, Martin, A: Action minima among solutions to a class of Euclidean scalar field equations. Commun. Math. Phys. 58, 211-221 (1978) MathSciNetView ArticleGoogle Scholar
  2. Berestycki, H, Lions, PL: Nonlinear scalar field equations, I. Existence of a ground state. Arch. Ration. Mech. Anal. 82, 313-345 (1983) MathSciNetMATHGoogle Scholar
  3. Bartsch, T, Willem, M: Infinitely many radial solutions of a semilinear elliptic problem on \(\mathbb{R}^{N}\). Arch. Ration. Mech. Anal. 124, 261-276 (1993) MathSciNetView ArticleMATHGoogle Scholar
  4. Liu, Z, Wang, ZQ: On the Ambrosetti-Rabinowitz superlinear condition. Adv. Nonlinear Stud. 4, 561-572 (2004) MathSciNetView ArticleMATHGoogle Scholar
  5. Ding, WY, Ni, WM: On the existence of positive entire solutions of a semilinear elliptic equation. Arch. Ration. Mech. Anal. 91, 283-308 (1986) MathSciNetView ArticleMATHGoogle Scholar
  6. Bartsch, T, Willem, M: Infinitely many nonradial solutions of a Euclidean scalar field equation. J. Funct. Anal. 117, 447-460 (1993) MathSciNetView ArticleMATHGoogle Scholar
  7. Fan, X: \(p(x)\)-Laplacian equations in \(\mathbb{R}^{N}\) with periodic data and nonperiodic perturbations. J. Math. Anal. Appl. 341, 103-119 (2008) MathSciNetView ArticleMATHGoogle Scholar
  8. Alves, CO, Liu, S: On superlinear \(p(x)\)-Laplacian equations in \(\mathbb{R}^{N}\). Nonlinear Anal. 73(8), 2566-2579 (2010) MathSciNetView ArticleMATHGoogle Scholar
  9. Ayoujil, A: On the superlinear Steklov problem involving the \(p(x)\)-Laplacian. Electron. J. Qual. Theory Differ. Equ. 36(38), 1 (2014) MathSciNetView ArticleMATHGoogle Scholar
  10. Dinca, G, Jebelean, P, Mawhin, J: Variational and topological methods for Dirichlet problems with p-Laplacian. Port. Math. 58, 339-378 (2001) MathSciNetMATHGoogle Scholar
  11. Bartsch, T, Liu, Z: On a superlinear elliptic p-Laplacian equation. J. Differ. Equ. 198, 149-175 (2004) MathSciNetView ArticleMATHGoogle Scholar
  12. Bonanno, G, Candito, P: Three solutions to a Neumann problem for elliptic equations involving the p-Laplacian. Arch. Math. (Basel) 80, 424-429 (2003) MathSciNetView ArticleMATHGoogle Scholar
  13. Ambrosetti, A, Rabinowitz, P: Dual variational methods in critical point theory and applications. J. Funct. Anal. 14, 349-381 (1973) MathSciNetView ArticleMATHGoogle Scholar
  14. Li, YQ, Wang, ZQ, Zeng, J: Ground states of nonlinear Schrödinger equations with potentials. Ann. Inst. Henri Poincaré, Anal. Non Linéaire 23, 829-837 (2006) MathSciNetView ArticleMATHGoogle Scholar
  15. Lions, PL: The concentration-compactness principle in the calculus of variations. The locally compact case. I. Ann. Inst. Henri Poincaré, Anal. Non Linéaire 1, 109-145 (1984) MathSciNetView ArticleMATHGoogle Scholar
  16. Lions, PL: The concentration-compactness principle in the calculus of variations. The locally compact case. II. Ann. Inst. Henri Poincaré, Anal. Non Linéaire 1, 223-283 (1984) MathSciNetView ArticleMATHGoogle Scholar
  17. Miyagaki, O, Souto, M: Superlinear problems without Ambrosetti and Rabinowitz growth condition. J. Differ. Equ. 245, 3628-3638 (2008) MathSciNetView ArticleMATHGoogle Scholar
  18. Struwe, M, Tarantello, G: On multivortex solutions in Chern-Simons gauge theory. Boll. Unione Mat. Ital., B 8, 109-121 (1998) MathSciNetMATHGoogle Scholar
  19. Liu, S: On superlinear problems without the Ambrosetti and Rabinowitz condition. Nonlinear Anal. 73, 788-795 (2010) MathSciNetView ArticleMATHGoogle Scholar
  20. Tan, Z, Fang, F: On superlinear \(p(x)\)-Laplacian problems without Ambrosetti and Rabinowitz condition. Nonlinear Anal. 75(9), 3902-3915 (2012) MathSciNetView ArticleMATHGoogle Scholar
  21. Gasinski, L, Papageorgiou, NS: Anisotropic nonlinear Neumann problems. Calc. Var. Partial Differ. Equ. 42, 323-354 (2011) MathSciNetView ArticleMATHGoogle Scholar
  22. Ge, B: On superlinear \(p(x)\)-Laplacian-like problem without Ambrosetti and Rabinowitz condition. Bull. Korean Math. Soc. 51(51), 409-421 (2014) MathSciNetMATHGoogle Scholar
  23. Carvalho, MLM, Goncalves, JVA, Silva, EDD: On quasilinear elliptic problems without the Ambrosetti-Rabinowitz condition. J. Math. Anal. Appl. 426(1), 466-483 (2015) MathSciNetView ArticleMATHGoogle Scholar
  24. Jones, C, Küpper, T: On the infinitely many solutions of a semilinear elliptic equation. SIAM J. Math. Anal. 17, 803-835 (1986) MathSciNetView ArticleMATHGoogle Scholar
  25. Rabinowitz, PH: Minimax Method in Critical Point Theory with Applications to Differential Equations. CBMS Reg. Conf. Ser. Math., vol. 65 (1986) View ArticleMATHGoogle Scholar
  26. Lions, PL: Symétrie et compactité dans les espaces de Sobolev. J. Funct. Anal. 49, 315-334 (1982) MathSciNetView ArticleMATHGoogle Scholar

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