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Existence and Asymptotic Profile of Nodal Solutions to Supercritical Problems

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Published/Copyright: December 21, 2016

Abstract

We establish the existence of nodal solutions to the supercritical problem

- Δ u = | u | p - 2 u in Ω , u = 0 on Ω ,

in a symmetric bounded smooth domain Ω of N, N3, for p>2N:=2NN-2, up to some range which depends on the symmetries, and we study their asymptotic behavior as p2N. We exhibit solutions up to this problem in symmetric domains with a shrinking hole, which concentrate at a single point as the hole shrinks and p approaches 2N from above, and whose limit profile is a rescaling of a nonradial sign-changing solution to the limit problem

- Δ u = | u | 2 N - 2 u , u D 1 , 2 ( N ) .

MSC 2010: 35J61; 35B33; 35B40

1 Introduction

We study the semilinear elliptic problem

(1.1) - Δ u = | u | p - 2 u in Ω , u = 0 on Ω ,

where Ω is a bounded smooth domain of N, N3, and p is either the critical Sobolev exponent 2N:=2NN-2 or it is supercritical, i.e., p>2N.

It is well known that, as a consequence of the classical Pohozaev identity, problem (1.1) does not admit, neither positive, nor sign-changing solutions, for these values of the exponent p, when Ω is starshaped.

For the critical case, many results concerning the existence and qualitative properties of solutions in nonstarshaped domains have been obtained in the last decades. A major breakthrough was achieved thanks to Abbas Bahri’s deep theory of critical points at infinity, which lead to the derivation of a fundamental existence result for problem (1.1) in domains with nontrivial topology, and to a delicate blow-up analysis for positive solutions to this problem, see [2, 3].

It is by now well understood that the solutions to the analogous problem in the whole of N,

(1.2) - Δ u = | u | 2 N - 2 u , u D 1 , 2 ( N ) ,

play a crucial role in the study of the critical problem (1.1), p=2N*. All positive solutions of (1.2) are known. They are obtained by rescaling a single radial solution, the so-called standard bubble, which is given explicitly. This explains why most existence results for the critical problem in bounded domains rely on constructions performed using the standard bubble as the basic cell, via variational or perturbation methods; see, e.g., [14] and the references therein.

Standard bubbles have been also used to construct positive solutions to the slightly supercritical problem (1.1), with p=2N+ε, for small enough ε>0, in domains with a small fixed hole [11, 10, 20] or with a shrinking hole [16]. As ε0, they blow up at two or more points of the domain in the first case, and at a single point inside the shrinking hole in the second case, and their limit profile at each blow-up point is a rescaling of the standard bubble. On the other hand, Ben Ayed and Bouh [4] showed that sign-changing solutions blowing up at two or three points which resemble a sum of positive and negative bubbles do not exist.

The existence of infinitely many sign-changing solutions to problem (1.2) was first established by Ding [13]. These solutions are invariant under the conformal action of groups, all of whose orbits are positive dimensional. Del Pino, Musso, Pacard and Pistoia [12] constructed other sign-changing solutions to (1.2) using positive and negative rescalings of the standard bubble as basic cells. In their recent paper [17], Musso and Wei used these solutions, in turn, as basic cells to construct sign-changing solutions to the slightly supercritical problem (1.1), with p=2N+ε, in a domain with a fixed small hole, for ε>0 sufficiently small. These solutions blow up at two different points of the domain as ε0, and their limit profile at each of these points is a rescaling of one of the sign-changing solutions of (1.2) constructed in [12].

Recently, new types of solutions to problem (1.2) were exhibited in [6], and it was shown that they arise as the limit profiles of solutions to subcritical problems (1.1), with particular symmetries, as p2N from below. These solutions are nonradial and change sign, and are quite different from those in [12]. In this paper we will show that they also arise as limit profiles of nodal solutions to the critical problem (1.1), p=2N*, in symmetric domains with a shrinking hole, see Theorem 4.2. These solutions are, therefore, different from the sign-changing solutions obtained in [8] for other types of symmetric domains, and from the bubble-towers constructed in [14]. Further, we will show that solutions to problem (1.2) of the type exhibited in [6] also arise as limit profiles of solutions to the supercritical problems (1.1), p>2N, as p2N from above.

To this end, we need first to consider the question of existence of solutions to the supercritical problem (1.1), p>2N. A fruitful approach, which has been applied in recent years to treat supercritical problems, consists in reducing them to some anisotropic critical or subcritical problem, either by considering rotational symmetries, or by means of maps which preserve the Laplace operator, or by a combination of both; see [9] for a detailed overview. These reductions apply only to some very specific types of domains Ω. A common feature of these domains is that they are invariant under the action of some group Γ whose orbits are positive dimensional. It turns out that this last condition suffices to establish existence. We will show that in a Γ-invariant domain Ω, problem (1.1) has infinitely many solutions for all p(2,2N-m), where m is the smallest dimension of a Γ-orbit in Ω and 2n:=2nn-2 is the critical Sobolev exponent in dimension n. Note that 2N<2N-m if m>0.

To avoid technicalities, here we only state a special case of this result. The general statement is given in Theorem 2.3 below.

Let 𝕊1:={eiϑ:ϑ[0,2π)} be the group of unit complex numbers, let O(m) be the group of linear isometries of m and let Aδ,R:={zN:0<δ<|z|<R} be an annulus. For N4, we write the points in N2×N-4 as (z,y) with z=(z1,z2)2, yN-4.

Theorem 1.1

Let N=4 or N6. Then, for every p(2,2N-1), the problem

(1.3) - Δ u = | u | p - 2 u in A δ , R , u = 0 on A δ , R ,

has infinitely many solutions which satisfy

(1.4) u ( z , y ) = u ( e i ϑ z , ϱ y ) 𝑎𝑛𝑑 u ( z 1 , z 2 , y ) = - u ( - z ¯ 2 , z ¯ 1 , y )

for all eiϑS1, ϱO(N-4), z=(z1,z2)C2 and yRN-4.

It is well known that problem (1.3) has one positive and infinitely many sign-changing radial solutions for every p(2,). Note, however, that the solutions provided by Theorem 1.1 are nonradial and change sign. For subcritical p(2,2N), the existence of infinitely many solutions satisfying (1.4) can be obtained by standard variational methods. For critical p=2N, this was shown in [6]. As in the critical case, for supercritical p(2N,2N-1), the symmetries play a crucial role.

The next theorem describes the asymptotic profile of the solutions provided by Theorem 1.1 as p approaches 2N from above and the hole shrinks. It is a special case of a more general result stated below; see Theorem 4.3.

Theorem 1.2

Fix R>0. For p(2N,2N-1), let uδ,p be a solution to (1.3) which satisfies (1.4) and has minimal energy among all solutions to (1.3) with these symmetry properties. Then there exist sequences (pk) in (2N,2N-1), and (δk) and (λk) in (0,), and a nontrivial solution ω to problem (1.2) such that the following hold:

  1. p k 2 N , δk0 and λk0.

  2. ω ( z , y ) = ω ( e i ϑ z , ϱ y ) and ω ( z 1 , z 2 , y ) = - ω ( - z ¯ 2 , z ¯ 1 , y ) for all e i ϑ 𝕊 1 , ϱO(N-4), z=(z1,z2)2 and yN-4. Also, ω has minimal energy among all solutions to (1.2) which have these symmetry properties.

  3. u δ k , p k has the following asymptotic profile:

    u δ k , p k = λ k 2 - N 2 ω ( λ k ) + o ( 1 ) in D 1 , 2 ( N ) .

We stress that the limit profile of the solutions uδ,p given by Theorem 1.2 is a rescaling of a nonradial sign-changing solution to problem (1.2), like those exhibited in [6]. So the solutions uδ,p are different from those constructed in [16], which resemble a rescaling of the standard bubble, and they are also different from the sign-changing solutions constructed in [17].

This paper is organized as follows. In Section 2, we describe the symmetries involved and we establish existence of infinitely many sign-changing solutions to problem (1.1) for supercritical exponents in some range which depends on the symmetries. In Section 3, we analyze the behavior of symmetric minimizing sequences for the critical problem. In Section 4, we describe the asymptotic profile of least energy symmetric solutions to the critical and the slightly supercritical problem in domains with a shrinking hole.

2 Symmetries and Compactness

Let Γ be a closed subgroup of the group O(N) of linear isometries of N, let Ω be a Γ-invariant bounded smooth domain in N, N3, and let ϕ:Γ/2:={1,-1} be a continuous homomorphism of groups such that {γΓ:γx0=x0}kerϕ for some x0Ω. This last condition guarantees that the space

D 0 1 , 2 ( Ω ) ϕ := { u D 0 1 , 2 ( Ω ) : u ( γ x ) = ϕ ( γ ) u ( x ) for all γ Γ , x Ω }

is infinite dimensional, cf. [5]. Here, as usual, D01,2(Ω) denotes the closure of 𝒞c(Ω) with respect to the norm

u := ( Ω | u | 2 ) 1 2 .

Let G:=kerϕ and set

D 0 1 , 2 ( Ω ) G := { u D 0 1 , 2 ( Ω ) : u ( g x ) = u ( x ) for all g G , x Ω } .

Note that D01,2(Ω)ϕD01,2(Ω)G. Note also that if ϕ is surjective and uD01,2(Ω)ϕ is nontrivial, then u changes sign.

The Sobolev embedding theorem and the Rellich–Kondrachov theorem imply that D01,2(Ω) is embedded in Lp(Ω) for every p[1,2N] and that this embedding is compact for p[1,2N), where 2n:=2nn-2 is the critical Sobolev exponent in dimension n. If every Γ-orbit in Ω has positive dimension and if we restrict to the space of G-invariant functions, the range of p’s for which this occurs increases. This was proved by Hebey and Vaugon in [15]. Their result is the core of the following proposition. Set

m := min { dim ( Γ x ) : x Ω } ,

where Γx:={γx:γΓ} is the Γ-orbit of the point x.

Proposition 2.1

If N-m>2, then D01,2(Ω)G and D01,2(Ω)ϕ are embedded in Lp(Ω) for every p[1,2N-m] and the embedding is compact for p[1,2N-m).

Proof.

Note that dim(Gx)=dim(Γx) for every xΩ. Hebey and Vaugon showed that the space D01,2(Ω)G is embedded in Lp(Ω) for every p[1,2N-m] and that the embedding is compact for p[1,2N-m), see [15, Corollary 2]. Since D01,2(Ω)ϕ is a subspace of D01,2(Ω)G, this is also true for D01,2(Ω)ϕ. ∎

Proposition 2.1 guarantees that the functional Jp:D01,2(Ω)G, given by

J p ( u ) := 1 2 u 2 - 1 p | u | p p ,

and the Nehari manifold

𝒩 p ϕ := { u D 0 1 , 2 ( Ω ) ϕ : u 0 , u 2 = | u | p p } ,

are well defined for p(2,2N-m], where ||p denotes the Lp-norm. It also guarantees that

c p ϕ := inf u 𝒩 ϕ J p ( u ) > 0 .

Now we consider problem (1.1) for p(2,2N-m]. A (weak) solution to this problem is a function uD01,2(Ω)Lp(Ω) such that

Ω u φ - Ω | u | p - 2 u φ = 0 for all φ 𝒞 c ( Ω ) .

Lemma 2.2

If p(2,2N-m] and u is a critical point of Jp:D01,2(Ω)ϕR, then u is a solution to problem (1.1) which satisfies

(2.1) u ( γ x ) = ϕ ( γ ) u ( x ) for all γ Γ , x Ω .

Proof.

For a function v:Ω and γΓ, we set vγ(x):=ϕ(γ)v(γ-1x). Since ϕ(γ-1gγ)=1 for every gG, we have that γ-1gγG. So, if vD01,2(Ω)G, then, as

v γ ( g x ) = ϕ ( γ ) v ( γ - 1 g x ) = ϕ ( γ ) v ( γ - 1 g γ γ - 1 x ) = ϕ ( γ ) v ( γ - 1 x ) = v γ ( x )

for every gG, we have that vγD01,2(Ω)G. This shows that D01,2(Ω)G is invariant under the action of Γ given by (γ,v)vγ. The set of fixed points of this action is the space D01,2(Ω)ϕ. Hence, by the principle of symmetric criticality, if u is a critical point of Jp:D01,2(Ω)ϕ, then u is also a critical point of Jp:D01,2(Ω)G, see [18].

For φ𝒞c(Ω), set

φ ~ ( x ) := 1 μ ( G ) G φ ( g x ) 𝑑 μ ,

where μ is the Haar measure. Then, φ~𝒞c(Ω)G:=𝒞c(Ω)D01,2(Ω)G. Since u is G-invariant, an easy computation shows that

Ω u φ ~ = Ω u φ and Ω | u | p - 2 u φ ~ = Ω | u | p - 2 u φ .

As u is a critical point of Jp:D01,2(Ω)G, this implies that

0 = J p ( u ) φ ~ = Ω u φ - Ω | u | p - 2 u φ for all φ 𝒞 c ( Ω ) ,

as claimed. ∎

Theorem 2.3

If p(2,2N-m), then problem (1.1) has a solution up, which satisfies (2.1) such that Jp(up)=cpϕ. Moreover, (1.1) has an unbounded sequence of solutions which satisfy (2.1).

Proof.

Since the embedding D01,2(Ω)ϕLp(Ω) is compact for p(2,2N-m), a standard argument shows that Jp satisfies the Palais–Smale condition on D01,2(Ω)ϕ. Therefore, cpϕ is attained on 𝒩pϕ and, as Jp:D01,2(Ω)ϕ is even and has the mountain pass geometry, the symmetric mountain pass theorem (see [1]) guarantees the existence of an unbounded sequence of critical values of Jp on 𝒩pϕ. By Lemma 2.2, the corresponding critical points are solutions to (1.1). ∎

The following example shows that this result is optimal. Let Ω:={(y,z)m+1×N-m-1:(|y|,z)B}, where B is an open ball centered in (0,)×{0}, whose closure is contained in the half-space (0,)×N-m-1. Note that Ω is invariant under the action of O(m+1) on the y-coordinate and m is the smallest dimension of an O(m+1)-orbit in Ω. In [19], Passaseo showed that (1.1) does not have a nontrivial solution for any p[2N-m,).

Proof of Theorem 1.1.

For N4, let Γ be the subgroup of O(N) generated by 𝕊1O(N-4){τ}, where eiϑ𝕊1, ϱO(N-4) and τ act on a point (z1,z2,y)××N-4N by

e i ϑ ( z 1 , z 2 , y ) := ( e i ϑ z 1 , e i ϑ z 2 , ϱ y ) ,
ϱ ( z 1 , z 2 , y ) := ( e i ϑ z 1 , e i ϑ z 2 , ϱ y ) ,
τ ( z 1 , z 2 , y ) := ( - z ¯ 2 , z ¯ 1 , y ) .

Let ϕ:Γ/2 be the homomorphism given by ϕ(eiϑ):=1=:ϕ(ϱ), ϕ(τ):=-1.

If N=4, then dim(Γx)=1 for every x=(z1,z2,y)Ar,R, whereas for N5, we have that

dim ( Γ x ) = { N - 4 if z 0 and y 0 , 1 if y = 0 , N - 5 if z = 0 .

Hence, m:=min{dim(Γx):xAr,R}=1 if N=4 and N6, and Theorem 1.1 follows from Theorem 2.3. ∎

To conclude this section, we study the continuity of cpϕ with respect to p(2,2N-m). We start with the following lemma.

Lemma 2.4

If pk,q(2,2N-m), pkq, and (uk) is a bounded sequence in D01,2(Ω)ϕ, then

lim k Ω ( | u k | p k - | u k | q ) = 0 .

Proof.

By the mean value theorem, for each xΩ, there exists qk(x) between pk and q such that

| | u k ( x ) | p k - | u k ( x ) | q | = | ln | u k ( x ) | | | u k ( x ) | q k ( x ) | p k - q | .

Fix η>0 so that [q-η,q+η](2,2N-m). Then, for some positive constant C and k large enough,

| ln | u k | | | u k | q k { ln | u k | | u k | q + η C | u k | 2 N - m if | u k | 1 , ( ln 1 | u k | ) | u k | q - η C | u k | 2 if | u k | 1 .

Therefore, using Proposition 2.1, we obtain

Ω ( | u k | p k - | u k | q ) = | u k | 1 ( | u k | p k - | u k | q ) + | u k | 1 ( | u k | p k - | u k | q )
C | p k - q | Ω ( | u k | 2 + | u k | 2 N - m )
C ¯ | p k - q | u k 2 N - m

for some positive constant C¯. As (uk) is bounded in D01,2(Ω), we conclude that limkΩ(|uk|pk-|uk|q)=0, as claimed. ∎

For p(2,2N-m), let up𝒩pϕ be a solution to (1.1) such that Jp(up)=cpϕ. Fix q(2,2N-m) and let tq,p(0,) be such that u~p:=tq,pup𝒩qϕ, i.e.,

(2.2) t q , p = ( u p 2 | u p | q q ) 1 q - 2 = ( | u p | p p | u p | q q ) 1 q - 2 .

Proposition 2.5

For q(2,2N-m), we have that

lim p q c p ϕ = c q ϕ , lim p q t q , p = 1 , lim p q J q ( u ~ p ) = c q ϕ .

Proof.

Set

S p ϕ := inf u D 0 1 , 2 ( Ω ) ϕ { 0 } u 2 | u | p 2 .

From Hölder’s inequality, we obtain that

S r ϕ | Ω | 2 ( r - p ) r p S p ϕ if p > r .

So, as p approaches q from the right, we get

lim sup p q + S p ϕ S q ϕ .

Assume that lim infpq+Spϕ<Sqϕ. Then there exist ε>0 and sequences (pk) in (q,2N-m) and (uk) in D01,2(Ω)ϕ, with |uk|pk=1, such that uk2<Sqϕ-ε. Lemma 2.4 implies that |uk|q1. Hence, uk2/|uk|q2<Sqϕ for k large enough, contradicting the definition of Sqϕ. This proves that

lim p q + S p ϕ = S q ϕ .

The corresponding statement when p approaches q from the left is proved in a similar way. Therefore, limpqSpϕ=Sqϕ. An easy computation shows that cpϕ=p-22p(Spϕ)pp-2. It follows that

c q ϕ = lim p q c p ϕ .

Since Jp(up)=p-22pup2=cpϕ, we have that (up) is bounded in D01,2(Ω)ϕ for p close to q. The expression (2.2), together with Lemma 2.4, yields limpqtq,p=1 which, in turn yields

lim p q J q ( u ~ p ) = lim p q q - 2 2 q t q , p u p 2 = lim p q t q , p 2 c p ϕ = c q ϕ ,

as claimed. ∎

3 Minimizing Sequences for the Critical Problem

Let ΩΓ:={xΩ:Γx={x}} be the set of Γ-fixed points in Ω. Throughout this section, we will assume that ΩΩΓ and ΩΓ are nonempty, and that every Γ-orbit in ΩΩΓ has positive dimension. We consider the critical problem

{ - Δ u = | u | 2 N - 2 u in Ω , u = 0 on Ω , u ( γ x ) = ϕ ( γ ) u ( x ) for all γ Γ , x Ω .

The solutions to this problem are the critical points of the energy functional J:D01,2(Ω)ϕ, given by

J ( u ) := 1 2 u 2 - 1 2 N | u | 2 N 2 N .

The nontrivial solutions lie on the Nehari manifold

𝒩 ϕ := { u D 0 1 , 2 ( Ω ) ϕ : u 0 , u 2 = | u | 2 N 2 N } .

We also consider the problem

(3.1) { - Δ u = | u | 2 N - 2 u , u D 1 , 2 ( N ) , u ( γ x ) = ϕ ( γ ) u ( x ) for all γ Γ , x N ,

and we denote by J:D1,2(N)ϕ its associated energy functional, and by 𝒩ϕ the corresponding Nehari manifold. We set

c ϕ := inf u 𝒩 ϕ J ( u ) and c ϕ := inf u 𝒩 ϕ J ( u ) .

The following nonexistence result was shown in [6].

Theorem 3.1

If ΩΓ, then cϕ=cϕ and cϕ is not attained by J on Nϕ.

Proof.

See [6, Theorem 2.3]. ∎

Theorem 3.3 below describes the shape of minimizing sequences for J on 𝒩ϕ. Its proof is similar to that of [6, Theorem 2.5]. We give a sketch of it here for the reader’s convenience.

Recall that the Γ-orbit Γx of a point xN is Γ-homeomorphic to the homogeneous space Γ/Γx, where

Γ x := { γ Γ : γ x = x }

is the isotropy group of x. In particular, #Γx=|Γ/Γx|, the index of the subgroup Γx in Γ.

Lemma 3.2

Given sequences (λk) in (0,) and (ξk) in RN, there exist a sequence (ζk) in RN and a closed subgroup K of Γ such that, after passing to a subsequence, the following statements hold true:

  1. The sequence ( λ k - 1 dist ( Γ ξ k , ζ k ) ) is bounded.

  2. Γ ζ k = K for all k .

  3. If | Γ / K | < , then λ k - 1 | α ζ k - β ζ k | for any α , β Γ with α - 1 β K .

  4. If | Γ / K | = , then there is a closed subgroup K of Γ such that KK, |Γ/K|= and λk-1|αζk-βζk| for any α,βΓ with α-1βK.

Proof.

See [7, Lemma 3.3]. ∎

Theorem 3.3

Assume that ΩΩΓ and ΩΓ are nonempty, and that every Γ-orbit in ΩΩΓ has positive dimension. Let(uk) be sequence in Nϕ such that J(uk)cϕ. Then, after passing to a subsequence, there exist a nontrivial solution ω to problem (3.1), a sequence (ζk) in ΩΓ and a sequence (λk) in (0,) with the following properties:

  1. λ k - 1 dist ( ζ k , Ω ) ,

  2. J ( ω ) = c ϕ ,

  3. lim k u k - λ k 2 - N 2 ω ( - ζ k λ k ) = 0 .

Proof.

By Ekeland’s variational principle, we may assume that (uk) is a Palais–Smale sequence. Then, (uk) is bounded in D01,2(Ω) and, after passing to a subsequence, uku weakly in D01,2(Ω). If u0, an easy argument shows that u𝒩ϕ and J(u)=cϕ, contradicting Theorem 3.1. Therefore, u=0.

Fix δ(0,N2cϕ). Then there exist bounded sequences (λk) in (0,) and (ξk) in N such that, after passing to a subsequence,

sup x N B λ k ( x ) | v k | 2 = B λ k ( ξ k ) | v k | 2 = δ .

For (λk) and (ξk), we choose K and (ζk) as in Lemma 3.2. Then, Γζk=K and dist(Γξk,ζk)<Cλk for some positive constant C and all k. Therefore, (ζk) is bounded and, as |vk| is Γ-invariant, we have that

(3.2) δ = B λ k ( ξ k ) | v k | 2 B ( C + 1 ) λ k ( ζ k ) | v k | 2 .

Set Ωk:={zN:λkz+ζkΩ} and, for zΩk, define

w k ( z ) := λ k N - 2 2 v k ( λ k z + ζ k ) .

The sequence (wk) is bounded in D1,2(N) so, after passing to a subsequence, wkω weakly in D1,2(N), wkω strongly in Lloc2(N), and wkω a.e. in N. A standard argument, using inequality (3.2), shows that ω0. Moreover, since Γζk=K, we have that wk(γz)=ϕ(γ)wk(z) for all γK. Hence,

(3.3) ω ( γ z ) = ϕ ( γ ) ω ( z ) for all γ K and all z N .

Using the fact that the equation -Δu=|u|2N-2u does not have a nontrivial solution in a half-space, it is also standard to show, after passing to a subsequence, that λk-1dist(ζk,Ω), ζkΩ and ω is a solution to -Δu=|u|2N-2u in N.

Now, if ζkΩΓ, then dim(Γζk)>0, and hence |Γ/K|=. But then, for any given m, statement (d) of Lemma 3.2 allows us to choose m elements α1,α2,,αmΓ such that λk-1|αjζk-αiζk| for ij. Arguing as in the proof of [6, inequality (2.7)], we obtain that

c ϕ m 1 N ω 2 .

This is a contradiction. Therefore, ζkΩΓ and K=Γ. From (3.3), we conclude that ω is a nontrivial solution to (3.1).

Note that

w k ( y - ζ k λ k ) = λ k N - 2 2 u k ( λ k y ) .

Since wkω weakly in D1,2(N), we have that

w k 2 = w k - ω 2 + ω 2 + o ( 1 )

and, performing the change of variable z=y-ζkλk, we obtain

N c ϕ = lim k u k 2 = lim k u k - λ k 2 - N 2 ω ( - ζ k λ k ) 2 + ω 2 ω 2 N c ϕ .

From Theorem 3.1, it follows that

lim k u k - λ k 2 - N 2 ω ( - ζ k λ k ) 2 = 0

and J(ω)=1Nω2=cϕ, as claimed. ∎

Theorem 3.3 asserts, in particular, the existence of a least energy nontrivial solution ω to problem (3.1). If ϕ1, ω is simply the standard bubble. On the other hand, if ϕ:Γ/2 is surjective, then ω is nonradial and sign-changing. Solutions of this type were recently exhibited in [6].

4 Minimizers of Critical and Slightly Supercritical Problems

Throughout this section, we continue to assume that ΩΩΓ and ΩΓ are nonempty, and that every Γ-orbit in ΩΩΓ has positive dimension. Set

d := min { dim ( Γ x ) : x Ω Ω Γ } .

Note that d1. Hence, 2N-d>2N. Set

Ω δ := { x Ω : dist ( x , Ω Γ ) > δ } ,

and fix δ0>0 so that Ωδ0.

For δ(0,δ0) and ε[0,2N-d-2N) we consider the problem

(4.1) { - Δ u = | u | 2 N - 2 + ε u in Ω δ , u = 0 on Ω δ , u ( γ x ) = ϕ ( γ ) u ( x ) for all γ Γ , x Ω δ .

This problem is critical for ε=0 and supercritical for ε>0. We write Jδ,ε:D01,2(Ωδ)ϕ for its associated energy functional,

𝒩 δ , ε ϕ := { u D 0 1 , 2 ( Ω δ ) ϕ : u 0 , u 2 = | u | 2 N + ε 2 N + ε }

for its Nehari manifold, and set

c δ , ε ϕ := inf u 𝒩 δ , ε ϕ J δ , ε ( u ) .

Extending each function in 𝒩δ,0ϕ by 0 outside Ωδ, we have that 𝒩δ,0ϕ𝒩ϕ and Jδ,0(u)=J(u) for every u𝒩δ,0ϕ, where 𝒩ϕ and J are the Nehari manifold and the energy functional associated to the critical problem in the whole domain Ω, as in the previous section. Hence, cϕcδ,0ϕ.

Lemma 4.1

We have that cδ,0ϕcϕ as δ0.

Proof.

For each η>0 there exists ψ𝒩ϕ𝒞c(Ω) such that J(ψ)<cϕ+η2. Let V:=(N)Γ be the space of Γ-fixed points in N and W:=V be its orthogonal complement. Our symmetry assumptions on Ω imply that dim(W)2. Hence, there are radial functions χk𝒞c(W) such that χk(y)=1 if |y|1k, χk(y)=0 if |y|2k and

lim k W | χ k ( y ) | 2 d y = 0 .

For (x,y)V×W, set ψk(x,y):=(1-χk(y))ψ(x,y). Then, supp(ψk)Ωδ if δ<1k. Note that, since χk is radial, we have

ψ k ( γ ( x , y ) ) = ψ k ( x , γ y ) = ( 1 - χ k ( γ y ) ) ψ ( x , γ y )
= ( 1 - χ k ( y ) ) ψ ( γ ( x , y ) ) = ϕ ( γ ) ( 1 - χ k ( y ) ) ψ ( x , y )
= ϕ ( γ ) ψ k ( x , y ) for all γ Γ .

Therefore, ψkD01,2(Ωδ)ϕ if δ<1k. Moreover, as

ψ - ψ k 2 = Ω | ( χ k ψ ) | 2 C 1 [ Ω Ω 2 / k χ k 2 | ψ | 2 + Ω ψ 2 | χ k | 2 ] C 2 [ | Ω Ω 2 / k | + W | χ k | 2 ] ,

we have that ψkψ in D01,2(Ω). Let tk(0,) be such that ψ~k:=tkψk𝒩ϕ. Clearly, ψ~kψ in D01,2(Ω). Hence, J(ψ~k)<cϕ+η for k large enough. Choosing k with this property and δ<1k, we conclude that ψ~k𝒩δ,0ϕ and cδ,0ϕJ(ψ~k)<cϕ+η. This finishes the proof. ∎

Theorem 2.3 asserts that, for δ(0,δ0) and ε[0,2N-d-2N), there exists a solution of (4.1) such that Jδ,ε(uδ,ε)=cδ,εϕ. The following results describe the asymptotic profile of these solutions, in the critical and the supercritical case, as δ0 and ε0.

Theorem 4.2

Let uδ be a solution to the critical problem (4.1), ε=0, such that Jδ,0(uδ)=cδ,0ϕ. Then there exist sequences (δk) and (λk) in (0,), a sequence (ζk) in ΩΓ and a nontrivial solution ω to

(4.2) Δ u = | u | 2 N - 2 u , u D 1 , 2 ( N ) ϕ ,

with the following properties:

  1. δ k 0 ,

  2. λ k - 1 dist ( ζ k , Ω ) ,

  3. J ( ω ) = c ϕ ,

  4. lim k u δ k - λ k 2 - N 2 ω ( - ζ k λ k ) = 0 .

Proof.

Since uδ𝒩δ,0ϕ𝒩ϕ and, by Lemma 4.1, we have J(uδ)cϕ as δ0, the result follows from Theorem 3.3. ∎

Theorem 4.3

For ε(0,2N-d-2N), assume that uδ,ε is a solution to the supercritical problem (4.1) such that Jδ,ε(uδ,ε)=cδ,εϕ. Then there exist sequences (δk), (εk) and (λk) in (0,), a sequence (ζk) in ΩΓ and a nontrivial solution ω to problem (4.2) with the following properties:

  1. δ k 0 , εk0,

  2. λ k - 1 dist ( ζ k , Ω ) ,

  3. J ( ω ) = c ϕ ,

  4. lim k u δ k , ε k - λ k 2 - N 2 ω ( - ζ k λ k ) = 0 .

Proof.

Let tδ,ε(0,) be such that u~δ,ε:=tδ,εuδ,ε𝒩δ,0ϕ𝒩ϕ. Proposition 2.5 allows us to choose ε(δ) in (0,2N-d-2N) with ε(δ)0 as δ0, such that u~δ:=u~δ,ε(δ) satisfies

c ϕ J ( u ~ δ ) = J δ , 0 ( u ~ δ ) c δ , 0 ϕ + δ .

By Lemma 4.1, we have that J(u~δ)cϕ as δ0. The result now follows from Theorem 3.3. ∎

Proof of Theorem 1.2.

This result is a special case of Theorem 4.3 applied to the ball Ω:={xN:|x|R}, with the action of the group Γ introduced in the proof of Theorem 1.1. Then ΩΓ:={0} and every Γ-orbit in ΩΩΓ has positive dimension if N=4 and N6. ∎


Dedicated to Abbas Bahri, a dear friend and an outstanding mathematician.



Communicated by Paul Rabinowitz


Funding statement: The research was supported by CONACYT grant 237661 and PAPIIT-DGAPA-UNAM grant IN104315 (Mexico), exchange funds of the Università “Sapienza” of Roma, and GNAMPA-INDAM funds (Italy).

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Received: 2016-11-11
Accepted: 2016-11-15
Published Online: 2016-12-21
Published in Print: 2017-02-01

© 2017 by De Gruyter

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

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