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BY 4.0 license Open Access Published by De Gruyter July 17, 2021

Existence and concentration of positive solutions for a critical p&q equation

  • Gustavo S. Costa and Giovany M. Figueiredo EMAIL logo

Abstract

We show existence and concentration results for a class of p&q critical problems given by

divaϵp|u|pϵp|u|p2u+V(z)b|u|p|u|p2u=f(u)+|u|q2uinRN,

where u ∈ W1,p(ℝN) ∩ W1,q(ℝN), ϵ > 0 is a small parameter, 1 < pq < N, N ≥ 2 and q* = Nq/(Nq). The potential V is positive and f is a superlinear function of C1 class. We use Mountain Pass Theorem and the penalization arguments introduced by Del Pino & Felmer’s associated to Lions’ Concentration and Compactness Principle in order to overcome the lack of compactness.

1 Introduction

In this paper we are concerned with a class of problems, named p&q problems type. In the last years the main interest in this general class of problems has been due to the fact that they arise from applications in physics and related sciences, such as biophysics, plasma physics and chemical reaction, as it can be seen for example in [20], [23] and [35]. In addition, such a class of problems encompasses a large class of problems, as can be seen in [4], [15] and [17].

More precisely, we show existence and concentration results of positive solutions for the critical problem given by

(Pε) divaϵp|u|pϵp|u|p2u+V(z)b|u|p|u|p2u=f(u)+|u|q2u in RN,uW1,pRNW1,qRN,

where ϵ > 0, N ≥ 2, 1 < pq < N and q* = Nq/(Nq). The hypotheses on the function a are the following: (a1)the function a is of class C1 and there exist constants k1, k2 ≥ 0 such that

k1tp+tqatptpk2tp+tq, for all t>0;

(a2)the mapping ta(tp)tqp is nonincreasing for t > 0;

(a3)if 1 < p < 2 ≤ N the mapping t a(t) is nondecreasing for t > 0. If 2 ≤ p < N the mapping tatptp2 is nondecreasing for t > 0.

As a direct consequence of (a2) we obtain that the map a and its derivative a satisfy

(1.1) a(t)t(qp)pa(t)for allt>0.

Now if we define the function h(t)=a(t)tqpA(t), using (1.1) we can prove that the function h is nonincreasing. Then, there exists a positive real constant γqp such that

(1.2) 1γa(t)tA(t),for allt0.

The hypotheses on the function b are the following:

(b1)The function b is of class C1 and there exist constants k3, k4 ≥ 0 such that

k3tp+tqb(tp)tpk4tp+tq,for allt>0;

(b2)the mapping tb(tp)tqp is nonincreasing for t > 0.

(b3)if 1 < p < 2 ≤ N the mapping t b(t) is nondecreasing for t > 0. If 2 ≤ p < N the mapping tbtptp2 is nondecreasing for t > 0.

Using the hypothesis (b2) and arguing as (1.1) and (1.2) we prove that there exists γqp such that

(1.3) 1γb(t)tB(t),for allt0.

The nonlinearity f is assumed to be a C1 function with the following hypotheses:

(f1)

lim|s|0f(s)|s|q1=0.

(f2) There exists q < r < q = q N N q such that

lim|s|f(s)|s|r1=0.

(f3) There exists θ(γp,q) such that

0<θF(s)f(s)sfors>0,

where F(s)=0sf(t)dt and γ > 0 was given in (1.2);

(f4) sf(s)sq1 is nondecreasing for s > 0.

(f5) There exist τ ∈ (q, q*) and λ > 1

f(s)λsτ1s>0.

We need to put some hypotheses on the potential V ∈ C(ℝN).

(V1)There is V0 > 0, such that

0 < V 0 V ( z ) for all z R N .

(V2)There exists a bounded domain Ω ⊂N such that

0 < V 0 = inf z Ω V ( z ) < inf z Ω V ( z ) .

In order to illustrate the degree of generality of the kind of problems studied here, with adequate hypotheses on the functions a and b, in the following we present more some examples of problems which are also interesting from the mathematical point of view and have a wide range of applications in physics and related sciences.

Problem 1

Let a(t)=1+tqpp and b(t)=1+tqpp. In this case we are studying problem

ΔpuΔqu+V(x)(|u|p2u+|u|q2u)=f(u)+|u|q2uinRN.

The Problem 1 comes from a general reaction–diffusion system: ut = div(Du∇u) + g(x, u), where Du:=[|u|p2+|u|q2]. In such applications, the function u describes a concentration, the term div(Du∇u) corresponds to the diffusion with a diffusion coefficient Du and g(·, u) is the reaction and relates to source and loss processes. Usually, in chemical and biological applications, the reaction term g(·, u) is a polynomial of u with variable coefficients.

Problem 2

Let a(t)=tqpp and b(t)=tqpp. In this case we are studying problem

ϵqΔqu+V(x)|u|q2u=f(u)+|u|q2uinRN

and it is related to the main result showed in [3] in the case q = 2. In [19] the author have studied the case 1 < q < N.

Problem 3

Let a(t)=1+1(1+t)p2pandb(t)=1. In this case we are studying problem

ϵ p div ( | u | p 2 u ) d i v ϵ p | u | p 2 u ( 1 + ϵ p | u | p ) p 2 p + V ( x ) | u | p 2 u = f ( u ) + | u | q 2 u in R N .

Problem 4

Let a(t)=1+tqpp+1(1+t)p2p and b(t)=1+tqpp. In this case we are studying problem

ϵ p Δ p u ϵ q Δ q u div ϵ p | u | p 2 u ( 1 + ϵ p | u | p ) p 2 p + V ( x ) ( | u | p 2 u + | u | q 2 u ) = f ( u ) + | u | q 2 u in R N .

The main result is the following:

Theorem 1.1

Suppose that a, b, f and V satisfy (a1)− (a3), (b1)− (b3), (f1)− (f5) and (V1)− (V2) respectively. Then there are ϵ0 > 0 and λ* > 1 such that (Pϵ) has a positive solution wϵ ∈ W1,p(ℝN) ∩ W1,q(ℝN), for every ϵ ∈ (0, ϵ0) and for every λ > λ*. In addition, if Pϵ is the maximum point of wϵ, then

limϵ0V(Pϵ)=V0.

Moreover, there are positive constants C and α such that

|wϵ(z)|Cexp(α|zPϵϵ|),

for all ϵ ∈ (0, ϵ0) and for all z ∈N.

In a seminal paper [31], Rabinowitz used his famous Mountain Pass Theorem(joint with Ambrosetti) [5] and showed the existence of solution for a Nonlinear Schrödinger Equation given by

(R) ϵ2Δu+V(x)u=f(u)inRN, u>0inRN,

where V is a continuous potential satisfying (V1) and

[(R1)]lim inf|x|V(x)=V, where V < ∞or V = ∞.

In [31], Rabinowitz used the force of the parameter ϵ and the geometry of the potential V in order to overcome the lack of compactness of Sobolev’s embedding to obtain the positive solution. In [33], Wang showed that the solution found by Rabinowitz concentrates around a local minimum of the potential V,when ϵ converges to zero. Wang also noted that the concentration of any family of solutions with energy uniformly bounded can only occur in a critical point of V. In [12], Del Pino and Felmer weakened the hypothesis (R1) of Rabinowitz and created a method that is known as Del Pino and Felmer’s penalization method.

As can be seen in [4], [15] and [17], p&q problems are generalizations of (R). However, as can seen below, we show that the arguments found in [12], [31] and [33] cannot be used directly. But before that, we are going to report some results on p&q problems type. There are interesting papers on such class of problems. We start with some problems in a bounded domain. For example, in [15] the author shows the existence and multiplicity of solutions for a critical p&q problem considering nonlinearity of type concave and convex. The critical case with discontinuous nonlinearities has studied in [16].

Now we comment some results in ℝN. Existence results was studied in [11] and [17]. In [2] the authors studied concentration results in Orlicz-Sobolev spaces with subcritical nonlinearity and the potential satisfying the local condition introduced by Del pino and Felmer [12]. In [4], it was showed the existence and concentration results with subcritical nonlinearity and the potential satisfying the global condition introduced by Rabinowitz [31]( see also [33]).

The present work is strongly influenced by the articles above. Below we list what we believe that are the main contributions of our paper.

  1. Unlike [4], [11] and [17], we show existence and concentration results considering the local hypothesis on potential introduced by Del Pino and Felmer [12].

  2. Unlike [2], we are considering the critical nonlinearity.

  3. Since the operator is not homogeneous, some estimates are different and more delicate than some estimates that can be found in [12] and [31] . For example, see Lemma 3.4, Proposition 5.1, Lemma 5.7 and all the Lemmas of Section 7.

  4. In order to overcome the lack of compactness provoked by the critical growth, it is very common to use the Talenti’s function (see [32]) to have some control on the minimax level, as can be seen in [10, Lemma 1.1]. The lack of homogenity of the p&q operator does not allow to use this argument. We overcome this difficulty using the solution of a problem in a bounded domain, as can be seen in Lemma 3.5.

The interest in the study of nonlinear partial differential equations with p&q operator or fractional p&q operator has increased because many applications arising in mathematical physics may be stated with an operator in this form. We cite the papers [6], [7], [8], [9], [18], [21], [22], [26], [27], [28], [29], [30] and their references. Several techniques have been developed or applied in their study, such as variational methods, fixed point theory, lower and upper solutions, global branching, and the theory of multivalued mappings.

This paper is organized as follows. In Section 2, we define an auxiliary problem using the penalization argument introduced by Del Pino and Felmer [12]. The existence of solution for the auxiliary problem was showed in Section 3. In order to show the concentration result, in Section 4 we studied the autonomous problem. The concentration result was showed in Section 5. In Section 6 we showed that the solutions of the auxiliary problem are solutions of the original problem. In Section 7 we showed the exponential decay of these solutions. To conclude the paper, we showed in an appendix the existence of a solution to a problem in a bounded domain that was important to overcome the lack of compactness.

2 Variational framework and an auxiliary problem

To prove Theorem 1.1, we will work with the problem below, which is equivalent to (Pϵ) by change variable z = ϵx, which is given by

(P~ε) divϵa|u|p|u|p2u+V(ϵx)b|u|p|u|p2u=f(u)+|u|q2u in RN,uW1,pRNW1,qRN,

where ϵ > 0, N ≥ 2 and 1 < pq < N.

In order to obtain solutions of (P˜ϵ), consider the following subspace of W1,p(RN)W1,q(RN) given by

W ϵ := { v W 1 , p ( R N ) W 1 , q ( R N ) : R N V ( ϵ x ) b ( | v | p ) | v | p d x < + } ,

which is a Banach space when endowed with the norm

u=u1,p+u1,q,

where

u 1 , m = R N | u | m d x + R N V ( ϵ x ) | u | m d x 1 m , for m 1.

Since the approach is variational, consider the energy functional associated Jϵ : Wϵ → ℝ given by

Jϵ(v)=1pRNA|v|pdx+1pRNV(ϵx)B|v|pdxRNF(v)dx1qRNv+qdx,

where u+ = max{u, 0}. By standard arguments, one can prove that Jϵ ∈ C1(Wϵ , ℝ). As we are interested in nonnegative solutions we can assume that f (s) = 0 for s ≤ 0.

Let β be a positive number satisfying β>maxpγθq(θpγ),V0pγq,1, where θ was given in (f3) and V0 appeared in (V1). From (f4), there exists η > 0 such that f(η)+ηq1ηq1=V0β. Then, using the above numbers,

we define the function of C1 class given by

f ~ ( s ) = 0 i f s 0 , f ( s ) + s q 1 i f 0 < s η 2 , V 0 β | s | q 2 s i f s > η .

We now define the function

g(z,s):=χΩ(z)[f(s)+(s+)q1]+(1χΩ(z))f˜(s),

and the auxiliary problem

(aux) divϵa|u|p|u|p2u+V(ϵx)b|u|p|u|p2u=g(ϵx,u) in RN,uWϵ

where χΩ is the characteristic function of the set Ω. It is easy to check that (f1)− (f4) imply that g is a Carathéodory function and for x ∈N, the function sg(ϵx, s) is of class C1 and satisfies the following conditions, uniformly for x ∈N:

(g1) lim|s|0g(ϵx,s)|s|q1=0
(g2) g(ϵx,s)f(s)+sq1,s>0andxRN
(g3)i 0<θG(ϵx,s)g(ϵx,s)s,ϵxΩands>0

and

(g3)ii 0 < q G ( ϵ X , s ) g ( ϵ X , s ) s 1 β V ( ϵ x ) | s | q , ϵ X Ω  and  s > 0 ,

where G(ϵx,s)=0sg(ϵx,t)dt.

The function

(g4) sg(ϵx,s)|s|q1is nondecreasing.

Remark 1

Note that, for z = ϵx, if uϵ is a positive solution of (Pϵaux ) with |uϵ(z)|η2 for every ϵx ∈N \ Ω, then uϵ(x) is also a positive solution of (Pϵ).

3 Existence of ground state for problem (Pϵaux)

Hereafter, let us denote by Iϵ : Wϵ → ℝ the functional given by

Iϵ(v)=1pRNA|v|pdx+1pRNV(ϵx)B|v|pdxRNG(ϵx,v)dx.

We denote by 𝒩ε the Nehari manifold of Iε, that is,

N ε := { u W ε { 0 } : I ε ( u ) , u = 0 }

and define the number bε by setting

(3.1) bε:=infuNεIε(u).

Using (f1), (f2) and (g2) we have: for every ξ > 0 there exists C ξ such that

(3.2) |g(εx,s)|ξ|s|q1+Cξ|s|r1+|s|q1for all xRN,sR.

Then, by definition of g and (3.2), there is rε > 0 such that

(3.3) urε>0for all uNε.

The main result in this section is:

Theorem 3.1

Let a satisfying (a1)−(a3), b satisfying (b1)−(b3), f satisfying (f1)−(f5) and V such that (V1)−(V2) hold. Then, there is λ* > 1 such that (Pϵaux ) has positive solution uϵW1,p(RN)W1,q(RN),foreveryλ>λ.

Moreover, we would like to highlight that in section 5, more precisely in Lemma 5.5, we are going to show that if Pϵϵ is the maximum point of uϵ then

limϵ0V(Pϵ)=V0.

In order to use the Mountain Pass Theorem [5], we define the Palais-Smale compactness condition. We say that a sequence (un) ⊂ Wϵ is a Palais-Smale sequence at level c for the functional Iϵ if

Iϵ(un)candIϵ(un)0in(Wϵ),

where

c:=infηΓmaxt[0,1]Iϵ(η(t))>0andΓ:={ηC([0,1],X):η(0)=0,Iϵ(η(1))<0}.

If every Palais-Smale sequence of Iϵ has a strong convergent subsequence, then one says that Iϵ satisfies the Palais-Smale condition ((PS) for short).

Lemma 3.2

The functional Iϵ : Wϵ → ℝ satisfies the following conditions

  1. There are α, ρ > 0 such that

Iϵ(u)α,ifu=ρ.

  1. For any uC0(Ωϵ,[0,)), we have

limtIϵ(tu)=.

Proof. Using (a1), (b1) and (3.2) we obtain

I ϵ ( u ) min { k 1 , k 3 } p u 1 , p p + 1 q u 1 , q q ξ p R N | u | p d x C ξ r R N | u | r d x 1 q R N | u | q d x .

By Sobolev embeddings, choosing ξ > 0 appropriate and taking ‖u‖ < 1 there are positive constants C1, C2, C3, such that

Iϵ(u)C1u1,pp+u1,qqC2urC3uqC4uqC2urC3uq.

Then the item (i) follows.

Now we show that the item (ii) holds. Consider a positive function wC0(Ωϵ),t>0 and using (a1), (b1), (f3) and Sobolev embedding, we have

Iϵ(tw)tppmax{k2,k4}w1,pp+tqqw1,qqtqqΩϵ|w|qdx.

This proves the second item.

Hence, there exists a Palais-Smale sequence (un) ⊂ Wϵ at level cϵ. Using (a2), (b2) and (f4), it is possible to prove that

c ϵ = b ϵ = inf u W ϵ { 0 } sup t 0 I ϵ ( t u ) ,

where bϵ was defined in (3.1).

In order to prove the Palais-Smale condition, we need to prove the next lemma.

Lemma 3.3

Let (un) be a (PS)d sequence for Iϵ, then the sequence (un) is bounded Wϵ. Moreover, for each ξ > 0 there exists R = R(ξ) > 0 such that

lim sup n R N B R ( 0 ) [ a ( | u n | p ) | u n | p + V ( ϵ x ) b ( | u n | p ) | u n | p ] d x < ξ .

Proof. Since (un) is a (PS)d sequence for functional Id, then using (1.1), (1.3), (g3)i and (g3)ii we have that

on(1)+d+on(1)un=Iϵ(un)1θIϵ(un)un1pγ1θRNa(|un|p)|un|p+1+μV(x)b(|un|p)|un|pdx1βRN|u|q+V(ϵx)|u|qdx1pγ1θmin{k1,k3}un1,pp+11βun1,qq.

Then, arguing as the [4, Lemma 2.3] , we can concluded that (un) is bounded in Wϵ.

Let ηR ∈ C(ℝN) be such that ηR(x) = 0 if x ∈ BR/2(0) and ηR(x) = 1 if xBR(0), with 0 ≤ ηR(x) ≤ 1 and |ηR|CR, where C is a constant independent of R. Since the sequence (ηRun) is bounded in Wϵ, and fixing R > 0 such that Ωϵ ⊂ B R/2(0) we obtain, by definition of the functional Iϵ,

R N B R ( 0 ) [ a ( | u n | p ) | u n | p + V ( ϵ x ) b ( | u n | p ) | u n | p ] d x = I ϵ ( u n ) u n η R + R N g ( ϵ x , u n ) u n η R d x R N u n a ( | u n | p ) | u n | p 2 u n η R d x + o n ( 1 ) .

Using (g3)ii we estimate

1 1 β R N B R ( 0 ) [ a ( | u n | p ) | u n | p + V ( ϵ x ) b ( | u n | p ) | u n | p ] d x R N | u n | a ( | u n | p ) | u n | p 1 | η R | d x + o n ( 1 ) .

As (un) is bounded in Wϵ and |ηR|CR. Passing to the limit in the last estimate, we get

lim sup n R N B R [ a ( | u n | p ) | u n | p + V ( ϵ x ) b ( | u n | p ) | u n | p ] d x < ξ .

for some R sufficiently large and for some fixed ξ > 0.

In the next result we show that the functional Iϵ satisfies the Palais-Smale condition for some levels. For this work we are denoting by S the best Sobolev constant for the embedding of D1,q(ℝN) into Lq(RN), that is, the largest positive constant S such that

(3.4) S R N | u | q d x q q R N | u | q d x for every u D 1 , q ( R N ) .

Lemma 3.4

The functional Iϵ satisfies the Palais-Smale condition at any level

d<1θ1qSN/q.

Proof. Let (un) ⊂ Wϵ be a Palais-Smale sequence at level d<1θ1qSN/q for the functional Iϵ. Arguing as Lemma [4, Lemma 2.3] we have that (un) is bounded in Wϵ. Then by Sobolev embeddings we deduce, up to a subsequence, that

(3.5) unuweakly inWϵ,un(x)u(x)q.t.pinRN,unustrongly inLlocs(RN)for anyps<q,un(x)u(x)for a.exRN.

Using the same kind of ideias contained [4, Lemma 2.3], we may conclude that u is a critical point of Iϵ. From Lemma 3.3 and for each ξ > 0 given there exists R > 0 such that

lim sup n R N B R ( 0 ) [ a ( | u n | p ) | u n | p + V ( ϵ x ) b ( | u n | p ) | u n | p ] d x < ξ .

This inequality, (a1), (b1), (f1), (f2), (g2) and the Sobolev embeddings imply, for n large enough, there exists a positive constant C1 such that

(3.6) R N B R ( 0 ) g ( ϵ x , u n ) u n d x C 1 ξ + ξ r / q + ξ q / q .

On the other hand, taking R large enough, we suppose that

(3.7) R N B R ( 0 ) g ( ϵ x , u ) u d x < ξ .

Therefore, by (3.6) and (3.7),

(3.8) R N B R ( 0 ) g ( ϵ x , u n ) u n d x = R N B R ( 0 ) g ( ϵ x , u ) u d x + o n ( 1 ) .

We claim that

(3.9) B R ( 0 ) ( R N Ω ϵ ) g ( ϵ x , u n ) u n d x = B R ( 0 ) ( R N Ω ϵ ) g ( ϵ x , u ) u d x + o n ( 1 ) .

Indeed, we have, in view of the definition of g,

g(ϵx,un)unf(un)un+η2q+V0β|un|qfor anyxRNΩϵ.

Since the set BR(0) (ℝNϵ) is bounded we can use the above estimate, (f1), (f2), (3.5) and Lebesgue’s Theorem to conclude that the convergence (3.9) holds.

Finally, we now prove the following convergence

(3.10) Ω ϵ | u n | q d x = Ω ϵ | u | q d x + o n ( 1 ) .

Since (un) is bounded in Wϵ and using the Lions’s Concentration Compactness Principle [25],wemay suppose that

|un|qμand|un|qν.

Then we obtain an at most countable index set Γ, sequences (xi) N and (μi), (νi) (0,∞), such that

(3.11) μ | u | q + i Γ μ i δ x i , ν = | u | q + i Γ ν i δ x i and S ν i q / q μ i ,

for all i ∈ Γ,where δxi is the Dirac mass at xiN. Thus it is sufficient to show that {xi}iΓΩϵ=. Then, we suppose by contradiction that xi ∈ Ωϵ for some i ∈ Γ. Consider R > 0 and the function ψR := ψ(xix), where ψC0(RN,[0,1]) is such that ψ ≡ 1 in BR(xi), ψ ≡ 0 in ℝN\B2R(xi), |∇ψ| ≤ 2, where R > 0 will be chosen in such way that the support of ψ is contained in Ωϵ. Then, as (ψRun) is bounded and Iϵ(un)ψRun=on(1),

R N u n a ( | u n | p ) | u n | p 2 u n ψ R d x + R N ψ R a ( | u n | p ) | u n | p d x + R N ψ R V ( ϵ x ) b ( | u n | p ) | u n | p d x = R N f ( x , u n ) ψ R u n d x + R N ψ R | u n | q d x + o n ( 1 ) .

Note that, using (a1), (b1) and that the function f has subcritical growth, we have

lim R 0 lim n R N u n a ( | u n | p ) | u n | p 2 u n p ψ R d x = 0 , lim R 0 lim n R N V ( ϵ x ) b ( | u n | p ) | u n | p ψ R d x = 0 ,

and

limR0limnRNf(x,un)ψRundx=0.

Therefore, by (a1) again,

R N ψ R | u n | q d x R N | u n | q ψ R d x + o n ( 1 ) .

Since ψR has compact support and letting n → ∞in the above expression, we see that

RNψRdμRNψRdν,

which implies

μiνi.

From this inequality and (3.11) one easily sees that SN/qνi.Asβ>pγθq(θpγ)andSN/qνi we have, by previous arguments,

d=Iϵ(un)1θIϵ(un)un+on(1)θpγpγθ1qβun1,qq+1θ1qΩϵ|un|qdx+on(1)1θ1qΩϵψR|un|qdx+on(1).

Hence, taking the limit and using (3.11), we get

d1θ1qiΓψR(xi)νi=1θ1qνi1θ1qSN/q

which does not make sense. Thus we obtain the convergence (3.10).

Therefore

(3.12) RNg(ϵx,un)undx=RNg(ϵx,u)udx+on(1).

Finally, we prove that, up to a subsequence, unu in Wϵ. Since Iϵ(un)un=on(1),Iϵ(u)=0 (3.12) and Fatou’s Lemma we have

0RNa(|un|p)|un|pa(|u|p)|u|pdx+RNV(ϵx)b(|un|p)|un|pb(|u|p)|u|pdx+RNg(ϵx,u)ug(ϵx,un)undx=on(1).

Then, using (a1) and (b1), we obtain ‖unu‖ = on(1), that is, the sequence (un) converges strongly to u.

For each fixed ϵ > 0, let us consider the following problem

(Pτ) k2ΔpuΔqu+Vk4|u|p2u+|u|q2u=|u|τ2u in Ωε,uW01,qΩϵ,

where τ is the constant which appears in the hypothesis (f5) and V:=maxxΩϵV(x) is a positive constant. We have associated to problem (Pτ) the functional

Iτ(u)=1pΩϵk2|u|p+Vk4|u|pdx+1qΩϵ|u|q+V|u|qdx1τΩϵ|u|τdx

and the associated Nehari manifold

Nτ={uW01,q(Ωϵ):u0andIτ(u)u=0}.

From Appendix there exists wτW01,q(Ωϵ) such that

Iτ(wτ)=cτ:=infuNτIτ(u),Iτ(wτ)=0

and

(3.13) c τ τ q τ q R N | w τ | τ d x .

Since λ is the parameter which appears in the hypothesis (f5) we have the following result.

Lemma 3.5

There exists λ* > 1, such that if λ>λ,thencϵ<(1θ1q)SN/q.

Proof. First of all, by the hypotheses (a1), (b1) and (f5), we obtain

R N a ( | w τ | p ) | w τ | p d x + R N V ( ϵ x ) b ( | w τ | p ) | w τ | p d x Ω ϵ k 2 | w τ | p + V k 4 | w τ | p d x + Ω ϵ | w τ | q + V | w τ | q d x = Ω ϵ | w τ | τ d x Ω ϵ f ( w τ ) w τ d x R N g ( ϵ x , w τ ) w τ d x ,

where V:=maxxΩϵV(x) This inequality implies that Iϵ(wτ±)wτ±0, and then there exists t ∈ (0, 1) such that twτ 𝒩ϵ. Using (a1), (b1) and (f5), we obtain

cϵIϵ(twτ)tppΩϵk2|wτ|p+Vk4|wτ|pdx+tqqΩϵ|wτ|q+V|wτ|qdxλτtτΩϵ|wτ|τdx.

Since t ∈ (0, 1), pq and Iϵ(wτ)wτ=0, we get

cϵIϵ(twτ)tppΩϵk2|wτ|p+Vk4|wτ|pdx+tppΩϵ|wτ|q+V|wτ|qdxλτtτΩϵ|wτ|τdx=tppλtττΩϵ|wτ|τdxmaxs0sppλsττΩϵ|wτ|τdx.

Using (3.13), we have

cϵmaxs0sppλsττcτqτ(τq)τppλp/(τp)cτq(τq)

By some straightforward algebric manipulations, we get

cϵτppλp/(τp)cτq(τq).

Then, if we choose λ>λ:=max1,[(τp)(τq)qpθq(qθ)cτSN/q](τp)/p in the hypothesis (f5), the proof is complete.

3.1 Proof of the Theorem 3.1

Proof. The proof is a consequence of Lemma 3.2, Lemma 3.4 and Lemma 3.5.

4 The Autonomous Problem

In order to prove the concentration result, we consider the following problem

(Po) diva|u|p|u|p2u+V0b|u|p|u|p2u=f(u)+|u|q1 in RNuW1,pRNW1,qRN

which the functional associated I0 is given by

I 0 ( u ) = 1 p R N [ A ( | u | p ) + V 0 B ( | u | p ) ] d x R N F ( u ) d x 1 q R N | u | q d x ,

and the corresponding Nehari manifold is given by

N 0 = { u W 1 , p ( R N ) W 1 , q ( R N ) { 0 } ; I 0 ( u ) u = 0 } .

We also define

c0=infN0I0.

Using the same arguments of the prove of Lemma 3.5, we conclude that

(4.1) c0<(1θ1q)SN/q.

The next result allows to show that problem (P0) has a solution that reaches c0.

Lemma 4.1

Let (un) 𝒩0 be a sequence such that I0(un)→ c0. Then there are a sequence (yn) N and constants R, η > 0 such that

(4.2) lim sup n B R ( y n ) | u n | q d x η .

Proof. Suppose that (4.2) is not satisfied. Since (un) is bounded in W1,p(ℝN) ∩ W1,q(ℝN) we have, by in [24, Lemma 2.1],

lim n R N | u n | s d x = 0 for all  s ( q , q ) .

Hence, from (f1)− (f3),

RNf(un)undx=on(1).

Since we also have (g3) and that Iϵn(un)un=on (1), we get

R N | u n | q d x = R N a ( | u n | p ) | u n | p d x + V 0 b ( | u n | p ) | u n | p d x + o n ( 1 ) := l

We claim that l > 0. Indeed, if the claim is not true then, by (a1) and (b1), we have c0 = 0 which is a contradiction. Therefore

(4.3) lim n R N | u n | q d x = l > 0.

By definition of the constant S, we have

(4.4) S R N | u n | q d x R N | u n | q d x q / q l q / N .

Thus, using (1.2), (1.3) and (f3), we deduce that

c 0 + o n ( 1 ) = I 0 ( u n ) 1 θ I 0 ( u n ) u n 1 θ 1 q R N | u n | q d x + o n ( 1 ) .

Using (4.3), (4.4) and that c0 > 0, we obtain c01θ1qSN/q which is a contradiction with (4.1).

We are going to show that the problem (P0) has a solution that reaches the level c0.

Lemma 4.2

(A Compactness Lemma) Let (un) 𝒩0 be a sequence satisfying I0(un) → c0. Then there exists a sequence (y˜n)RN such that, up to a subsequence, vn(x)=un(x+y˜n) converges strongly in W1,p(ℝN) ∩ W1,q(ℝN). In particular, there exists a minimizer for c0.

Proof. Applying Ekeland’s Variational Principle (see Theorem 8.5 in [34]),wemay suppose that (un) is a (PS)c0 for I0. Since (un) is bounded in W1,p(ℝN) ∩ W1,q(ℝN) we can assume, up to subsequences, that un ⇀ u in W1,p(ℝN) ∩ W1,q(ℝN).

Using arguments found in [4, Lemma 2.3], we have that

(4.5) un(x)u(x)a.einRNandI0(u)=0.

Then, by (1.2), (1.3) and the Fatou’s Lemma,

01pRNA(|u|p)+V0B(|u|p)dx1θRNa(|u|p)|u|p+V0B(|u|p)|u|pdxlim infn+1pRNA(|un|p)+V0B(|un|p)dx1θRNa(|un|p)|un|p+V0B(|un|p)|un|pdx

Hence, if u ∈ 𝒩0,

c0I0(u)1θI0(u)ulim infn+I0(un)1θI0(un)un=limn+I0(un)=c0.

By (4.5), (a1), (b1) and Lebesgue’s theorem we conclude that unuinW1,p(RN)W1,q(RN). Consequently, I0(u) = c0 and the sequence (y˜n) is the null sequence.

If u ≡ 0, then in that case we cannot have unu strongly in W1,p(ℝN) ∩ W1,q(ℝN) because cV0 > 0. Hence, using Lemma 4.1, there exists a sequence {y˜n} N such that

vnvinW1,p(RN)W1,q(RN),

where vn:=un(x+y˜n). Therefore, (vn) is also a (PS)c0 sequence for I0 and v/0. It follows from the above arguments that, up to a subsequence, (vn) converges strongly in W1,p(ℝN) ∩ W1,q(ℝN) and the proof is complete.

5 Concentration results

In this section we prove some technical results in order to show the concentration result.

Proposition 5.1

Let ϵn → 0 and (un) 𝒩ϵn be such that Iϵn (un)→ c0. Then there exists a sequence (y˜n) N such that vn(x)=un(x+y˜n) has a convergent subsequence in W1,p(ℝN) ∩ W1,q(ℝN). Moreover, up to a subsequence, yny ∈ Ω, where yn=ϵny˜n.

Proof. Since V satisfies (V1) and c0 > 0, we repeat the same arguments in Lemma 4.1 to conclude that there exist positive constants R andβ˜ and a sequence (y˜n)RN such that

lim infnBR(y˜n)unqβ˜>0.

Since the sequence (un) is bounded in W1,p(ℝN) ∩ W1,q(ℝN) we immediately obtain, up to a subsequence, vnv/0 in W1,p(ℝN) ∩ W1,q(ℝN), where vn(x):=un(x+y˜n). Let tn > 0 be such that

(5.1) v˜n=tnvnN0.

Then, since unNϵn, we have

(5.2) c0I0(v˜n)Iϵn(v˜n)Iϵn(vn)=Iϵn(un)=c0+on(1),

which implies that I0(v˜n)c0, as n → +∞.

From boundedness of (vn) and (5.2), we obtain that (tn) is bounded. As a consequence, the sequence (v˜n) is also bounded in W1,p(ℝN) ∩ W1,q(ℝN) which implies, up to a subsequence, v˜nv˜ weakly in W1,p(ℝN) ∩ W1,q(ℝN).

Note that we can assume that tnt0 > 0. Then, this limit implies that v˜/0. From Lemma 4.2, we conclude that vn˜v˜ in W1,p(ℝN) ∩ W1,q(ℝN) and this implies that vnv in W1,p(ℝN) ∩ W1,q(ℝN).

To conclude the proof of this proposition, we consider yn:=ϵny˜n. Our goal is to show that (yn) has a subsequence, still denoted by (yn), satisfying yny for y ∈ Ω. First of all, we claim that (yn) is bounded. Indeed, suppose that there exists a subsequence, still denote by (yn), verifying | yn| → ∞. From(a1), (b1) and (V1) we have

RNk1|vn|p+|vn|qdx+V0RNk3|vn|p+|vn|qdxRNg(ϵnx+yn,vn)vndx.

Fix R > 0 such that BR(0) ⊃ Ω and let 𝒳BR(0) be the characteristic function of BR(0). Since XBR(0)(ϵx+yn)=on(1) for all x ∈ BR(0) and vnv in W1,p(ℝN) ∩ W1,q(ℝN), then

RNXBR(0)(ϵx+yn)g(ϵx+yn,vn)vndx=on(1).

By definition off˜ we obtain that

RNk1|vn|p+|vn|qdx+V0RNk3|vn|p+|vn|qdxRNBR(0)f˜(vn)vndx+on(1)V0βRN|vn|qdx+on(1).

It follows that vn → 0 in W1,p(ℝN) ∩ W1,q(ℝN), obtain this way a contradiction because c0 > 0.

Hence (yn) is bounded and, up to a subsequence,

ynyRN.

Arguing as above, if yˉΩˉ we will obtain again vn → 0 in W1,p(ℝN) ∩ W1,q(ℝN), and then yΩ. Now if V(y) = V0, we have y/Ω and consequently y ∈ Ω. Suppose by contradiction that V(y)>V0. Then, we have

c0=I0(v˜)<1pRNA(|v˜|p)dx+1pRNV(y)B(|v˜|p)dxRNF(v˜)dxRN|v˜|qdx.

Using the fact that v˜nv˜ in W1,p(ℝN) ∩ W1,q(ℝN), from Fatou’s Lemma we obtain

c0<lim infn[1pRNA(|v˜n|p)dx+1pRNV(ϵnz+yn)B(|v˜n|p)dxRNF(v˜n)dxRN|v˜n|qdx.]

Since unNϵn, this implies that

c0<lim infnIϵn(tnun)lim infnIϵn(un)=c0,

obtaining a contradiction.

Lemma 5.2

Let (ϵn) be a sequence such that ϵn → 0 and (un)Nϵn a solution of problem (Pϵaux) . Then (vn) converges uniformly on compacts ofN, where vn(x):=un(x+y˜n). Moreover, given ξ > 0, there exist R > 0 and n0 N such that

v n L ( R N B R ( 0 ) ) < ξ for all n n 0 ,

where (y˜n) is the sequence of Proposition 5.1.

Proof. Note that vn is a solution of problem

divavnpvnp2vn+Vϵx+ynbvnpvnp2vn=gϵx+yn,vn in RN,vnWϵ,

where yn=ϵny˜n. Adapting some arguments explored in [4, Lemma 5.5], we have that the sequence (vn) is bounded in L(ℝN) and there exist R > 0 and n0 N such that

vnL(RNBR(0)<ξ,for allnn0.

Then, for any bounded domain Ω N, from (g1)− (g2) and continuity of V there exists C > 0 such that

|V(ϵx+yn)vnp1g(ϵx+yn,vn)|C,for allnN.

Hence,

|V(ϵx+yn)vnp1g(ϵx+yn,vn)|C+|vn|p,for allnN.

Considering Ψ(x) = C, we get that ΨLt(Ω) with t>pp1N. From [13, Theorem 1], we have

vnLloc(RN).

Therefore, for all compact K ⊂ Ω there exists a constant C0 > 0, dependent only on C, N, p and dist(K,Ω), such that

|vn|,KC0.

Then,

|vn|Cloc0,ν(RN)C,for allnNand0<ν<1.

From Schauder’s embedding, (vn) has a subsequence convergent in Cloc0,ν(RN).

Lemma 5.3

Given ϵ > 0, the solution uϵ of problem (Pϵaux) satisfies

limϵ0Iϵ(uϵ)=cV0.

Proof. Consider z0 ∈ Ω such that V(z0) = V0. Let us now consider R > 0 and set Q ∈ ∂BR(z0). If necessary, take R small enough such that B(Q, R/4) ⊂ Ω. Taking ψ : ℝN → ℝ such that ψ ≡ 1 in B(Q, R/4) and ψ ≡ 0 in ℝN\B(Q, R/2).

Let w0 ∈ W1,p(ℝN) ∩ W1,q(ℝN) be a ground-state positive solution of the problem (P0) which satisfies c0 = I0(w0) (see Lemma 4.2). Then, we consider the function wϵ : ℝN → ℝ be given by

wϵ(x):=ψi(ϵx)w0xz0ϵWϵ

and tϵ > 0, such that tϵwϵ 𝒩ϵ. Then, with a direct computation, we have

Iϵ(uϵ)Iϵ(tϵwϵ)=c0+oϵ(1).

Finally, taking R → 0 in the last inequality and using the continuity of the minimax function (see [1], [31]) we get

lim supϵ0Iϵ(uϵ)c0.

Let tϵ,0 > 0 be such that tϵ,0uϵ 𝒩0. Then,

c0I0(tϵ,0uϵ)Iϵ(tϵ,0uϵ)Iϵ(uϵ)

and the proof is complete.

Lemma 5.4

Let (ϵn) be a sequence such that ϵn → 0 and for each n ∈ N, let (un) 𝒩ϵn be a solution of problem (Pϵaux). Then, there are δ* > 0 and n0 N such that, for vn(x)=un(x+y˜n), we have

vn(x)δ,forallxBR(0)andnn0,

where R > 0 and (y˜n) were given in Lemma 5.2.

Proof. Suppose, by contradiction, that u n L ( | x | < R ) = u n L x y ~ n < R 0. By Lemma 5.2, we have vnL(RN)0. It follows from (f1) that

(5.3) |f(vn)+vnq1|V02|vn|q1fornsufficient large.

Thus,

RNa(|vn|p)|vn|pdx+RNV(ϵnx+yn)b(|vn|p)|vn|pdx=RNf(vn)vndx+on(1)V02RN|vn|qdx+on(1),

which implies from (a1) and (b1) that,

unWϵn0,

which is a contradiction with Lemma 5.3.

We are now ready to show the concentration of the ground state solution.

Lemma 5.5

If Pϵϵ is the maximum point of uϵ, then

limϵ0V(Pϵ)=V0.

Proof. We first notice that using Lemma 5.4 there exist δ* > 0 and n0 N such that

vn(qn):=maxzRNvn(z)=un(qn+y˜n)un(x)δ, for all nn0, for all x ∈ BR(0).

We claim that (qn) is bounded, otherwise using Lemma 5.2 and 5.4, there exists R* > 0 such that vnL(RNBR)δ2, which implies that |vn(qn)|δ2, where we obtain a contradiction.

Then, Pϵn=ϵnqn+yn which implies

limn+Pϵn=limn+yn=yΩ.

Hence from continuity of V it follows that

limn+V(Pϵn)=V(y)V0.

We claim that V(y)=V0. Indeed, suppose by contradiction that V ( y ¯ ) > V 0 . Then, we have

c0=I0(v˜)<1pRNA(|v˜|p)dx+1pRNV(y)B(|v˜|p)dxRNF(v˜)1qRN|v˜|qdx.

Using that v˜nv˜inW1,p(RN)W1,q(RN) we obtain, from Fatou’s Lemma,

c0<lim infn[1pRNA(|v˜n|p)dx+1pRNV(ϵnz+yn)B(|v˜n|p)dxRNF(v˜n)1qRN|v˜n|qdx],

and therefore

c0<lim infnIϵn(tnun)lim infnIϵn(un)=c0.

This contradiction shows that V(y)=V0.

Lemma 5.6

Let {ϵn} be a sequence of positive numbers such that ϵn → 0 as n → ∞and let (xn)Ωϵn be a sequence such that uϵn (xn)≥ Υ > 0for some constant Υ, where for each nN,uϵn is a solution of (Pϵaux). Then,

limnV(xn)=V0

where xn=ϵnxn.

Proof. Up to a subsequence,

xnxΩ.

From Lemma 5.3 we have that

Iϵn(uϵn)c0,

and there exists a positive constant C such that

uϵnC,nN,for someC>0.

Setting vn(z):=uϵn(z+xn),we havevnCandvnvinW1,p(RN)W1,q(RN). Recalling that

vn(0)=uϵn(xn)Y>0,

we conclude that v/0.

Fix tn > 0 verifying v˜n=tnvnN0, for each n ∈ N. Hence,

c0I0(v˜n)Iϵn(tnvn)Iϵ(vn)=Iϵ(un)=c0+on(1).

Thus, I0(v˜n)c0, with {v˜n}N0. By Lemma 4.2, we have

(5.4) v˜nv˜inW1,p(RN)W1,q(RN)andI0(v˜)=c0.

Since v˜0, by Proposition 5.1 we have yn = 0, for n ∈ N. Moreover, recalling that V is continuous, we have

limnV(xn)=V(x).

We claim that V(x)=V0. Indeed, Suppose by contradiction that V(x)> V0, then

c0=I0(v˜)<1pRNA(|v˜|p)dx+1pRNV(x)B(|v˜|p)dxRNF(v˜)dx1qRN|v˜|qdx.

Thus, by (5.4) and Fatou’s Lemma, we have

c 0 < lim inf n 1 p A R N v ~ n p d x + 1 p V R N ϵ n z + x ¯ n B v ~ n p d x F R N v ~ n d x 1 q R N | v ~ | q d x lim inf n 1 p A R N t n v n p d x + 1 p V R N ϵ n z + x ¯ n B t n v n p d x G R N ϵ n z + x ¯ , t n v n d x = lim inf n I ϵ n t n u n lim inf n I ϵ n u n = c 0 ,

which leads a absurd. Consequently limnV(xn)=V0.

Lemma 5.7

If mϵ is given by mϵ=sup{maxΩϵuϵ: is a solution of (Pϵaux)}, then there exists ϵ>0 such that the sequence (mϵ) is bounded for all ϵ(0,ϵ). Moreover, we have limϵ0mϵ=0.

Proof. Suppose, by contradiction, limϵ0mϵ=+, then there exist uϵ a solution of (Pϵaux) in 𝒩ϵ and Υ > 0 such that

maxΩϵuϵY>0

Thus there exists n}⊂+ with ϵn → 0 and there exists a sequence {xn}Ωϵn such that

uϵn(xn)Y>0.

Thus, by Lemma 5.6, we have

limnV(xn)=V0,

where xn=ϵnxnand {xn}Ω. Hence, up to a subsequence, we have xnx in ∂Ω and V(x)=V0, which does not make sense by (V2). Hence, there exists ϵ > 0 such that (mϵ) is bounded, for all ϵ(0,ϵ).

Suppose by contradiction that there exists δ > 0 and a sequence n}⊂+ satisfying

mϵnδ>0

Thus, there exists uϵn a solution of (Pϵaux ) such that

mϵnδ2<maxΩϵnuϵnmϵn.

Hence,

δ2=δδ2mϵnδ2<maxΩϵuϵn,

and then there exists a sequence (xn) ⊂ ∂Ωϵn , such that

uϵn(xn)δ2.

Repeating the above arguments, we will get an absurd. Thus, the proof is finished.

6 Proof of Theorem 1.1

Proof. Let uϵ be a solution of (Pϵaux). By Lemma 5.7, there exists ϵ>0 such that mϵ<η2 for all ϵ(0,ϵˉ), then (uϵη2)+(x)0 for a neighborhood from ∂Ωϵ. Hence, (uϵη2)+W01,p(RNΩϵ)W01,q(RNΩϵ) and the function (uϵη2)+W1,p(RN)W1,q(RN), where

(uϵη2)+(x):=0ifxΩϵ,(uϵη2)+(x)ifxRNΩϵ.

Using (uϵη2)+ as test function. Then, by (a1), (b1) and (g3)ii, we have

0RNΩϵa(|uϵ|p)|(uϵη2)+|pdx+RNΩϵ[V0b(|uϵ|p)|uϵ|p2V0β|uϵ|q2]((uϵη2)+)2dx+RNΩϵ[V(ϵx)b(|uϵ|p)|uϵ|p2V0β|uϵ|q2]η2(uϵη2)+dx=0

The last equality implies

(uϵη2)+=0,a.e inxRNΩϵ.

This implies that |uϵ|η2 for z ∈Nϵ, and by Remark 1 the result follows.

7 Exponential decay of the solution uϵ

Finally, we are going to prove the exponential decay. First technical results

Lemma 7.1

Consider M, α > 0 and ψ(x) := Mexp(−α|x|). Then

i)div(a|ψ|p|ψ|p2ψ)=αp1pαp+1a(αpψp)ψ2p1+a(αpψp)ψp1(N1)|x|α(p1),ii)div(a|ψ|p|ψ|p2ψ)(N1)|x|α(q1)a(αpψp)αp1ψp1.

Proof. Note that

ψxi(x)=Mexp(α|x|)xi(α|x|)=Mexp(α|x|)(α)xi|x|=αxi|x|ψ(x),

which implies |∇ψ| = αψ. Then

div(a|ψ|p|ψ|p2ψ)=i=1Nxia|ψ|p|ψ|p2ψxi=αp1i=1Nxiaαpψpψp1xi|x|=αp1i=1Naαpψpxiαpψpψp1xi|x|+a(αpψp)xiψp1xi|x|=αp1i=1Naαpψpαppψ2p2ψxixi|x|+a(αpψp)|x|2xi2|x|3ψp1+(p1)ψp2ψxixi|x|=αp1pαp+1a(αpψp)ψ2p1+a(αpψp)ψp1(N1)|x|α(p1),

this prove the first item.

To prove the item ii) we are going to use (1.2) and the item i).Hence we have

a(αpψp)αpψp(qp)pa(αpψp),

and consequently

pαp+1a(αpψp)ψ2p1αψp1(qp)a(αpψp).

Therefore, by the item i),

div(a|ψ|p|ψ|p2ψ)αp1α(qp)a(αpψp)ψp1+(N1)|x|α(p1)a(αpψp)ψp1=(N1)|x|α(q1)a(αpψp)αp1ψp1.

Corollary 7.2

Since V(x) ≥ V0 inN, then for α > 0 small enough we have

div(a|ψ|p|ψ|p2ψ)+k3V0ψp1+V04ψq10inRN.

Proof. Using (a1) and Lemma 7.1 we obtain that

div(a|ψ|p|ψ|p2ψ)α(q1)a(αpψp)αp1ψp1α(q1)k2αp1ψp1+αq1ψq1=α(q1)k2αp1ψp1α(q1)αq1ψq1

Moreover, since V0 > 0 and α > 0 is small enough, we concluded that

k3V0α(q1)k2αp10

and

V04α(q1)αq10.

Consequently

div(a|ψ|p|ψ|p2ψ)+k3V0ψp1+V04ψq10inRN.

Let us now relate the positive solution vϵ to the exponential function ψ for small ϵ.

Lemma 7.3

Let uϵ be the solution found in Theorem 3.1 and vϵ(x):=uϵ(x+y˜ϵ) given in Proposition 5.1. For φϵ = max{vϵψ, 0} and ϵ > 0 sufficient small, we have

RNa(|vϵ|p)|vϵ|p2vϵφϵdx+k3V0RN|vϵ|p1φϵdx+V04RN|vϵ|q1φϵdx0.

Proof. From Lemma 5.2, Lemma 5.3 and hypothesis (f1), there exist ρ0 > 0 such that ϵ > 0 small enough,

f(vϵ)+vϵq1|vϵ|q134V0, for all|x|ρ0.

Since ψ(x) := Mexp(−α|x|) for x ∈N, we can find M˜>0 such that if MM˜, then φϵ:=max{|vi,ϵ|ψ,0}0 in Bρ0(0) and φϵ ∈ W1,p(|x|ρ0) ∩ W1,q(|x|ρ0). Therefore, the above inequality and (b1),

RNa(|vϵ|p)|vϵ|p2vϵφϵdx+V0RNk3|vϵ|p1φϵ+|vϵ|q1φϵdxRNa(|vϵ|p)|vϵ|p2vϵφϵdx+RNV(ϵx+yϵ)b(|vϵ|p)|vϵ|p2vϵφϵdxRNf(vϵ)φϵdx3V04RN|vϵ|q1φϵdx

and the lemma is proved.

Finally we are going to show the exponential decay for the functions uϵ.

Proposition 7.4

There are ϵ0 > 0 and C > 0 such that

|uϵ(z)|Cexp(α|zPϵϵ|),forallzRN.

Proof. From [14, Lemma 2.4], we have that

a(|x|p)|x|p2xa(|y|p)|y|p2y,xy0,x,yRN.

Consider vϵ(x):=uϵ(x+y˜ϵ) the set

Λ:={xRN:|x|ρ0and|vϵ|ψ0},

where ψ is the function is given by Lemma 7.1, (y˜n) is given by Proposition 5.1. Then, using Corollary 7.2 and Proposition 7.3, we obtain

0RNa(|vϵ|p)|vϵ|p2vϵa(|ψ|p)|ψ|p2ψ,φ˜dx+V0k3RN|vϵ|p1|ψ|p1φ˜dx+V04RN|vϵ|q1|ψ|q1φ˜dxV0k3RN|vϵ|p1|ψ|p1φ˜dx+V04RN|vϵ|q1|ψ|q1φ˜dx=V0k3Λ|vϵ|p1|ψ|p1(vϵψ)dx+V04Λ|vϵ|q1|ψ|q1(vϵψ)dx0.

Then |Λ| = 0 and consequently

vϵ(x)Mexp(α|x|),|x|ρ0.

Considering x=zy˜ϵ and using Lemma 5.5 there exists a constant C > 0 satisfying

(7.1) |uϵ(z)|Mexpαzyϵϵ=MexpαzPϵ+ϵqϵϵMexpαzPϵϵexpαqϵCexpαzPϵϵ,

for all |zy˜ϵ|ρ0 and for ϵ > 0 small enough.

Now we are going to show the inequality (7.1) holds, for all z ∈N. Since (yϵ) converges, it follows that

|z|ρ0|yϵ˜|=ρ0|yϵ|ϵ>ρ01+|yϵ|ϵasϵ0.

Then, there exists ϵ0 > 0 such that

|uϵ(z)|CexpαzPϵϵ,zRNandϵ(0,ϵ0).

Appendix

In this appendix we are going to show the existence of positive solution for a problem in a bounded domain with smooth boundary, denoted by Ω. More precisely, we are going to study the following problem

k2ΔpuΔqu+Vk4|u|p2u+V|u|q2u=|u|τ2uinΩu=0onΩ,(Pτ)

where Ω is a bounded domain in ℝN and k2, k4, V are positive constants. We have associated to problem (Pτ) the functional

Iτ(u)=1pΩk2|u|p+Vk4|u|pdx+1qΩ|u|q+V|u|qdx1τΩ|u|τdx

and the Nehari manifold

Nτ={uW01,q(Ω):u0andIτ(u)u=0}

Lemma 7.5

For all uW01,q(Ω){0} there exists a unique tu (0, +∞), such that tu ∈ 𝒩τ.

Proof. Note that if uW01,q(Ω){0} and t > 0, we have

Iτ(tu)=tτtpτpΩk2|u|p+Vk4|u|pdx+tqτqΩ|u|q+V|u|qdx1τΩ|u|τdx.

Then,

limt0Iτ(tu)tτ=+andlimt+Iτ(tu)tτ=1τΩ|u|τdx<0.

Consequently, there exists tu (0, +∞) such that Iτ(tuu)=supt0Iτ(tu) and tuu ∈ 𝒩τ.

In order to show the unicity of tu, consider f (t) = tτ and note that f(t)tq is increasing.

Lemma 7.6

The following properties hold:

  1. There exists ρτ > 0 such that Ω|u|qdx1/qρτ,foralluNτ;

  2. There exists a constant Cτ > 0 such that Iτ(u)CτΩ|u|qdx, for all u ∈ 𝒩τ.

Proof. By Sobolev’s embeddings, there exists C > 0 such that

Ω|u|qdxΩk2|u|p+Vk4|u|pdx+Ω|u|q+V|u|qdx=Ω|u|τdxCΩ|u|qdxτ/q.

Since τ > q, the item (i) follows.

To verify the second assertion observe that

Iτ(u)=Iτ(u)1τIτ(u)u1p1τΩk2|u|p+Vk4|u|pdx+1q1τΩ|u|q+V|u|qdx1q1τΩ|u|qdx.

Proposition 7.7

There exists wτW01,q(Ω) such that wτ is a solution of (Pτ) and I τ ( w τ ) = inf N τ I τ .

Proof. Let (un) be a minimizing sequence for Iτ in 𝒩τ. By Lemma 7.6, we conclude that (un) is bounded in W01,q(Ω). Then there exists uW01,q(Ω) such that, up to a subsequence, unuinW01,q(Ω) and

(7.2) unustrongly inLs(Ω)for any1s<q,un(x)u(x)for a.exΩ.

Since τ ∈ (q, q*) we have, by Lemma 7.6 again, that u ≠0. Hence,

cτIτ(tuu)lim infnIτ(tuun)lim infnIτ(un)+on(1)=cτ.

Considering wτ := tuu we have Iτ(wτ) = cτ and using Implicit Theorem we conclude that Iτ(wτ)=0.

Acknowledgements

Gustavo S. Costa and Giovany M. Figueiredo were partially supported by CNPq, Capes and FAPDF - Brazil.

  1. Conflict of interest: Authors state no conflict of interest.

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Received: 2021-03-07
Accepted: 2021-05-10
Published Online: 2021-07-17

© 2021 Gustavo S. Costa and Giovany M. Figueiredo, published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

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