Abstract

We consider the existence of nontrivial solutions to elliptic equations with decaying cylindrical potentials and subcritical exponent. We will obtain a local minimizer by using Ekeland’s variational principle.

1. Introduction

In this paper, we study the existence of nontrivial solutions of the following problem:where , and let and be integers such that and belongs to . is the critical Sobolev exponent, , , is a continuous function on , and and are parameters which we will specify later.

We denote point in by the pair , , and , the closure of with respect to the norms with for .

From the Hardy inequality, it is easy to see that the norm is equivalent to .

We define the weighted Sobolev space with , which is a Banach space with respect to the norm defined by .

My motivation of this study is the fact that such equations arise in the search for solitary waves of nonlinear evolution equations of the Schrödinger or Klein-Gordon type (cf. [1–3]). Roughly speaking, a solitary wave is a nonsingular solution which travels as a localized packet in such a way that the physical quantities corresponding to the invariances of the equation are finite and conserved in time. Accordingly, a solitary wave preserves intrinsic properties of particles such as the energy, the angular momentum, and the charge, whose finiteness is strictly related to the finiteness of the -norm. Owing to their particle-like behavior, solitary waves can be regarded as a model for extended particles and they arise in many problems of mathematical physics, such as classical and quantum field theory, nonlinear optics, fluid mechanics, and plasma physics (see, e.g., [4]).

Several existence and nonexistence results are available in the case , and we quote, for example, [5–7] and the references therein. When , ; problem has been studied in the famous papers by Brézis and Nirenberg [8] and Xuan [9] which consider the existence and nonexistence of nontrivial solutions to quasilinear Brézis-Nirenberg-type problems with singular weights.

Concerning the existence result in the case , we cite [10, 11] and the references therein. As noticed in [10], for and , Badiale and Rolando have considered the problem . They established the existence of nontrivial nonnegative radial solution when and or and ; in addition, if the function is odd, then has infinitely many radial solutions. In [5], Badiale et al. proved the nonexistence of nonzero classical solutions when and the pair belongs to the light gray region. That is, , where

Since our approach is variational, we define the functional on by We say that is a weak solution of the problem if it is a nontrivial nonnegative function and satisfies Throughout this work, we consider the following regions , , such that with .

Concerning the perturbation , we assume In our work, we prove the existence of at least one critical point of by Ekeland’s variational principle in [12].

We will state our main result.

Theorem 1. Assume that , , , and hold.
If , then there exists such that the problem has at least one nontrivial solution for any .

This paper is organized as follows. In Section 2, we give some preliminaries. Section 3 is devoted to the proof of Theorem 1.

2. Preliminaries

We list here a few integrals inequalities. The first inequality that we need is the weighted Hardy inequality [13] The starting point for studying is the Hardy-Sobolev-Maz’ya inequality that is peculiar to the cylindrical case and that was proved by Gazzini and Musina in [14]. It states that there exists positive constant such that for ; equation of is related to a family of inequalities given by Caffarelli et al. [15], for any . The embedding is compact, where and is the weighted space with respect to the norm

Definition 2. Assume , , and . Then, the infimum defined by is achieved on .

Lemma 3. Let be a Palais-Smale sequence ( for short) of such thatfor some . Then, in and .

Proof. From (10), we have where denotes as . Then, and is bounded in . Going if necessary to a subsequence, we can assume that there exists such that Consequently, we get, for all , which means that

3. Existence Result

Firstly, we require the following lemmas.

Lemma 4. Let be a sequence of for some . Then, and either

Proof. We know that is bounded in . Up to a subsequence if necessary, we have that Denote , and then . As in Brézis and Lieb [16], we have From Lebesgue theorem and by using the assumption , we obtain Then, we deduce that From the fact that in , we can assume that Assuming that , we have by definition of and so Then, we get Therefore, if not, we obtain . That is, in .

Lemma 5. Suppose that , , and hold. If , then there exist and and positive constants such that, for all ,(i)there exist such that ,(ii)we have

Proof. (i) Let where is small, and such that . Choosing , then, if large enough, Thus, if , we obtain that .
(ii) By the Holder inequality and the definition of and since , we get for all If , then there exist and small enough such that We also assume that is small enough such that . Thus, we have Using Ekeland’s variational principle, for the complete metric space with respect to the norm of , we can prove that there exists a sequence such that for some with .
Now, we claim that . If not, by Lemma 4, we have which is a contradiction.
Then, we obtain a critical point of for all large enough satisfying

Proof of Theorem 1. From Lemmas 4 and 5, we can deduce that there exists at least a nontrivial solution for our problem with positive energy.

Conflict of Interests

The author declares that there is no conflict of interests regarding the publication of this paper.