In this paper, we are concerned with a class of fractional Robin problems with variable exponents. Their main feature is that the associated Euler equation is driven by the fractional p(⋅)−Laplacian operator with variable coefficient while the boundary condition is of Robin type. This paper is a continuation of the recent work established by A. Bahrouni, V. Radulescu and P. Winkert [
Citation: Ramzi Alsaedi. Infinitely many solutions for a class of fractional Robin problems with variable exponents[J]. AIMS Mathematics, 2021, 6(9): 9277-9289. doi: 10.3934/math.2021539
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In this paper, we are concerned with a class of fractional Robin problems with variable exponents. Their main feature is that the associated Euler equation is driven by the fractional p(⋅)−Laplacian operator with variable coefficient while the boundary condition is of Robin type. This paper is a continuation of the recent work established by A. Bahrouni, V. Radulescu and P. Winkert [
Fractional Sobolev spaces have major applications to various nonlinear problems, including phase transitions, thin obstacle problem, anomalous diffusion, crystal dislocation, semipermeable membranes and flame propagation, ultra-relativistic limits of quantum mechanics, minimal surfaces, water waves, etc. For more details, we refer the readers to Di Nezza, Palatucci and Valdinoci [21]. More recently, the works of Caffarelli et al. [9,10,11], led to a large amount of papers involving the fractional diffusion operator (−Δ)s (0<s<1). The cited results turn out to be very fruitful in order to recover an elliptic PDE approach in a nonlocal framework, and they have recently been used very often, see [1,6,7,16,18,24,26,27]. We mention that there are also a great number of results which do not survive in the fractional framework, such as the ones mentioned in [13,14].
On the other hand, the study of PDE's involving variable exponents has become very attractive in recent decades, see [15,17,19,23,25,30] and the references therein.
It is therefore a natural question to see which results "survive" when the p(x)−Laplacian is replaced by the fractional p(x)−Laplacian.
As far as we know, the first result about the fractional Sobolev spaces with variable exponent of the form Ws,q(⋅),p(⋅,⋅)(Ω) and the fractional p(x)−Laplacian is obtained by Kaufmann-Rossi-Vidal in [22]. In particular it is shown that theses spaces are compactly embedded into variable exponent Lebesgue spaces. They also study the existence existence of solution for nonlocal problems involving the fractional p(⋅,⋅)−Laplacian. Bahrouni-Radulescu [2] obtained some further qualitative properties of the fractional Sobolev spaces and the fractional p(⋅,⋅)−Laplacian. Further developments have been done by Bahrouni, Ho, Biswas, Chung, Zhang, see [3,4,5,8,12,20,29].
The main goal of this paper is to study the existence of infinitely many solutions for fractional p(⋅,⋅)−Laplacian equation with nonlocal Robin boundary condition. Precisely, we deal with the following problem
(−Δ)sp(⋅,⋅)u+|u|¯p(x)−2u=a(x)|u|q(x)−2uin Ω,Ns,p(⋅,⋅)u+β(x)|u|¯p(x)−2u=0in RN∖¯Ω, | (1.1) |
where Ω⊂RN, N>1, is a bounded domain with Lipschitz boundary, a,q∈L∞(Ω), s∈(0,1), p:R2N→(1,+∞) is a symmetric, continuous function bounded away from 1, ¯p(⋅)=p(⋅,⋅), β∈L∞(RN∖Ω) with β≥0 in RN∖Ω and (−Δ)sp(⋅,⋅) stands for the fractional p(⋅,⋅)−Laplacian which is given by
(−Δ)sp(⋅,⋅)u(x)=p. v.∫RN|u(x)−u(y)|p(x,y)−2(u(x)−u(y))|x−y|N+sp(x,y)dyfor x∈Ω. | (1.2) |
Furthermore, Ns,p(⋅,⋅) is defined by
Ns,p(⋅,⋅)u(x)=∫Ω|u(x)−u(y)|p(x,y)−2(u(x)−u(y))|x−y|N+sp(x,y)dyfor x∈RN∖¯Ω, | (1.3) |
and denotes the nonlocal normal p(⋅,⋅)-derivative (or p(⋅,⋅)−Neumann boundary condition) and describes the natural Neumann boundary condition in presence of the fractional p(⋅,⋅)−Laplacian. We would like to mention that the nonlocal normal derivative was introduced for the first time by A. Bahrouni, V. Radulescu and P. Winkert in [5]. This paper can be considered as a continuation of this study. Precisely, using variational methods, we will prove the existence of infinitely many solutions of Eq (1.1).
Now, we recall some results obtained by U. Kaufmann et al. [22]. Let Ω be a bounded Lipschitz domain in RN, s∈(0,1), q∈C(¯Ω,R), and p∈C(¯ΩׯΩ,R). Throughout this paper, we assume that
1<p(x,y)=p(y,x)<Ns, ∀(x,y)∈¯Ω×¯Ω | (P') |
and
1<q(x)<Np(x,x)N−sp(x,x)=:p∗s(x), ∀x∈¯Ω. | (Q') |
We define the fractional Sobolev space with variable exponents Ws,q(⋅),p(⋅,⋅)(Ω) as
Ws,q(⋅),p(⋅,⋅)(Ω)={u∈Lq(⋅)(Ω): ∃ λ>0, ∫Ω×Ω|u(x)−u(y)|p(x,y)λp(x,y)|x−y|N+sp(x,y)dxdy<∞}. |
Let
[u]s,p(⋅,⋅),Ω=inf{λ>0: ∫Ω×Ω|u(x)−u(y)|p(x,y)λp(x,y)|x−y|N+sp(x,y)dxdy≤1} |
be the corresponding variable exponent Gagliardo seminorm. For brevity, we denote Ws,q(⋅),p(⋅,⋅)(Ω) by E for a general q∈C(¯Ω,R) satisfying (Q') and by Ws,p(⋅,⋅)(Ω) when q(x)=p(x,x) on ¯Ω. We equip E with the norm
‖u‖E=[u]s,p(⋅,⋅),Ω+‖u‖Lq(⋅)(Ω). |
Then, E becomes a reflexive and separable Banach space.
Now, we are ready to recall a crucial theorem which prove some embedding results was obtained in [22] for the case q(x)>p(x,x) on ¯Ω and then was refined in [20,29].
Theorem 1.1. Let Ω⊂RN be a bounded Lipschitz domain and let s∈(0,1). Let p∈C(¯ΩׯΩ,R) and q∈C(¯Ω,R) satisfy (P') and (Q') with q(x)≥p(x,x) for all x∈¯Ω. Let r∈C(¯Ω,R) satisfy
1<r(x)<p∗s(x), ∀x∈¯Ω. | (R) |
Then, there exists a constant C=C(N,s,p,q,r,Ω) such that
‖f‖Lr(⋅)(Ω)≤C‖f‖E, ∀f∈E. |
Thus, E is continuously embedded in Lr(⋅)(Ω). Moreover, this embedding is compact.
From Theorem 1.1 and using assumptions (P') and (Q') with q(x)≥p(x,x) for all x∈¯Ω, we can deduce that spaces E and Ws,p(⋅,⋅)(Ω) actually coincide. Evidently, E is not suitable for studying the fractional p(.,.)−Laplacian problem with Robin boundary condition and hence, we need to introduce another space as our solution space.
We suppose the following assumptions:
(A) a∈L∞(Ω) and a>0 in Ω.
(S) s∈R with s∈(0,1);
(P) p:R2N→(1,+∞) is a symmetric, continuous function bounded away from 1, that is,
p(x,y)=p(y,x)for all x,y∈R2N |
with
1<p−:=min(x,y)∈R2Np(x,y)≤p(x,y)≤p+:=max(x,y)∈R2Np(x,y). |
and sp+<N;
(β) β∈L∞(RN∖Ω) and β≥0 in RN∖Ω;
Let u:RN→R be a measurable function and let ¯p(x)=p(x,x) for all x∈R2N. We set
‖u‖X:=[u]s,p(⋅,⋅),R2N∖(CΩ)2+‖u‖L¯p(⋅)(Ω)+‖β1¯p(⋅)u‖L¯p(⋅)(CΩ), |
where CΩ=RN∖Ω and
X:={u:RN→R measurable : ‖u‖X<∞}. |
(X,‖⋅‖X) is a reflexive and separable Banach space, see [5]. Let us recall the compact embedding result introduced in [22].
Proposition 1.2. Assume that (S), (P) and (β) hold. Then, for any r∈C(¯Ω) with 1<r(x)<p∗s(x) for all x∈¯Ω, there exists a constant α>0 such that
‖u‖Lr(⋅)(Ω)≤α‖u‖Xfor allu∈X. |
Moreover, this embedding is compact.
Now we give our main result.
Theorem 1.3. Assume that q(x)∈(1,p−), for all x∈Ω and conditions (A), (S), (P) and (β) are fulfilled. Then problem (1.1) has infinitely many solutions.
This paper is organized as follows. In Section 2 we recall some definitions and fundamental properties of the spaces Lp(⋅)(Ω) and W1,p(⋅)(Ω). In Section 3 we give the proof of Theorem 1.3.
In this section, we recall some definition and basic properties concerning the basic function spaces with variable exponent. We refer to [5,15,17,23,25,30] and the references therein.
We start by giving a bounded Lipschitz domain Ω⊂RN. Next, we consider the following set
C+(¯Ω)={p∈C(¯Ω,R):p(x)>1forallx∈¯Ω}. |
For any p∈C+(¯Ω), denote
p+=supx∈Ωp(x)andp−=infx∈Ωp(x) |
and recall the variable exponent Lebesgue space Lp(⋅)(Ω) as
Lp(⋅)(Ω)={u: u is measurable real-valued function, ∫Ω|u(x)|p(x)dx<∞}, |
which is endowed with the following Luxemburg norm
‖u‖Lp(⋅)(Ω)=inf{μ>0:∫Ω|u(x)μ|p(x)dx≤1}. |
It is well known that (Lp(⋅)(Ω),‖⋅‖Lp(⋅)(Ω)) is a separable reflexive Banach space.
The variable exponent Sobolev space W1,p(⋅)(Ω) is defined by
W1,p(⋅)(Ω)={u∈Lp(⋅)(Ω):|∇u|∈Lp(⋅)(Ω)} |
with the norm
‖u‖1,p(⋅)=‖∇u‖p(⋅)+‖u‖p(⋅). |
Let Lq(⋅)(Ω) be the conjugate space of Lp(⋅)(Ω), that is, 1/p(x)+1/q(x)=1 for all x∈¯Ω. If u∈Lp(⋅)(Ω) and v∈Lq(⋅)(Ω), then the Hölder-type inequality
|∫Ωuvdx|≤(1p−+1q−)‖u‖p(⋅)‖v‖q(⋅) |
is satisfied.
Defining the modular function ρ:Lp(⋅)(Ω)→R by
ρ(u)=∫Ω|u|p(x)dx. |
Then, we have the following crucial result which will be useful in the sequel.
Proposition 2.1. Assume that u∈Lp(⋅)(Ω). Then:
(i) ‖u‖p(⋅)<1(=1,>1)⟺ρ(u)<1(=1,1);
(ii) ‖u‖p(⋅)>1 ⇒ ‖u‖p−p(⋅)≤ρ(u)≤‖u‖p+p(⋅);
(iii) ‖u‖p(⋅)<1 ⇒ ‖u‖p+p(⋅)≤ρ(u)≤‖u‖p−p(⋅)\.
Proposition 2.2. Assume that u,un∈Lp(⋅)(Ω) with n∈N. Then the following statements are equivalent:
(i) limn→+∞‖un−u‖p(⋅)=0;
(ii) limn→+∞ρ(un−u)=0;
(iii) un(x)→u(x) a. e. in Ω and limn→+∞ρ(un)=ρ(u).
Now, we introduce the variational setting for problem (1.1). We define the functional I:X→R by
I(u)=∫R2N∖(CΩ)2|u(x)−u(y)|p(x,y)2p(x,y)|x−y|N+sp(x,y)dxdy+∫Ω|u|¯p(x)¯p(x)dx+∫CΩβ(x)|u|¯p(x)¯p(x)dx−∫Ωa(x)q(x)|u|q(x)dx, |
which is well defined and of class C1 on X. Clearly, the weak solutions of our main problem (1.1) are exactly the critical points of the Euler-Lagrange functional I.
In this section, we investigate the existence of infinitely many solutions for problem (1.1). It is known that, by [19], there exist (en)⊂X and e∗n⊂X∗ such that
e∗n(em)=1 if n=m and e∗n(em)=0 if n≠m. |
It follows that
X=¯span{en, n≥1} and X∗=¯span{e∗n, n≥1}. |
For any integer k≥1, denote
Ek=span{ek}, Yk=⊕kj=1Ej and Zk=¯⊕∞j=kEj. |
Consider now the functional
Iλ(u)=J(u)−λK(u), |
where
J(u)=∫R2N∖(CΩ)2|u(x)−u(y)|p(x,y)2p(x,y)|x−y|N+sp(x,y)dxdy+∫Ω|u|¯p(x)¯p(x)dx+∫CΩβ(x)|u|¯p(x)v¯p(x)dx |
and
K(u)=∫Ωa(x)|u(x)|q(x)q(x)dx. |
An important ingredient in the proof of Theorem 1.3 is the following version of the fountain theorem, see Zou [31].
Theorem 3.1. Suppose that the functional Iλ defined above satisfies the following conditions:
(T1) Iλ maps bounded sets to bounded sets uniformly for λ∈[1,2]. Furthermore, Iλ(−u)=Iλ(u) for all (λ,u)∈[1,2]×X;
(T2) K(u)≥0, K(u)→∞ as ‖u‖→∞ on any finite dimensional subspace of X;
(T3) there exist ρk>rk>0 such that
ak(λ):=infu∈Zk,‖u‖=ρkIλ(u)≥0>bk(λ)=maxu∈Yk,‖u‖=rkIλ(u)for λ∈[1,2], |
dk(λ)=infu∈Zk,‖u‖≤ρkIλ(u)→0as k→∞ uniformly for λ∈[1,2]. |
Then there exist a sequence of real numbers (λn) converging to 1 and u(λn)∈Yn such that I′λn|Yn(uλn)=0 and (Iλn)(u(λn))→ck∈[dk(2),bk(1)] as n→∞. In particular, fixed k∈N, if (u(λn)) has a convergent subsequence to uk, then I1 has infinitely many nontrivial critical points (uk)⊂X∖{0} satisfying I1(uk)→0− as k→∞.
We start with the following auxiliary property.
Lemma 3.2. Suppose that condition (A) is satisfied. Then
βk=supu∈Zk,‖u‖=1∫Ωa(x)|u(x)|q(x)q(x)dx→0 as k→+∞. |
Proof. It is easy to see that 0<βk+1≤βk, so that βk→β≥0 as k→+∞. For every k≥0, by definition of βk, there exists uk∈Zk such that ‖uk‖=1 and ∫Ωa(x)|uk|q(x)q(x)dx>βk2. Since uk∈Zk, it follows that uk⇀0 in X. From Proposition 1.2, we deduce that ∫Ωa(x)|uk|q(x)q(x)dx→0 as k→+∞. Thus, β=0 and the proof is complete.
Next, we prove the coercivity of K on finite dimensional subspaces of X.
Lemma 3.3. Suppose that conditions of Theorem 1.3 are fulfilled. Then K(u)→+∞ as ‖u‖→+∞ on any finite dimensional subspace of X.
Proof. Let F be a finite dimensional subspace of X. Put
˜a(x)=a(x)q(x), ∀x∈Ω. |
First we show that there exists ϵ1>0 such that
m{x∈Ω; ˜a(x)|u|q(x)≥ϵ1‖u‖q(x)}≥ϵ1, ∀u∈F∖{0}. | (3.1) |
Arguing by contradiction, for any positive integer n, there exists un∈F∖{0} such that
m{x∈Ω; ˜a(x)|un|q(x)≥1n‖un‖q(x)}<1n. | (3.2) |
Set vn(x)=un(x)‖un‖∈F∖{0}. Then ‖vn‖=1 for all n∈N and
m{x∈Ω; ˜a(x)|vn|q(x)≥1n}<1n. |
We may assume, up to a subsequence, that vn→v0 in X for some v0∈F. Then ‖v0‖=1 and, by Proposition 1.2,
∫Ω˜a(x)|vn−v0|q(x)dx→0 as n→+∞. | (3.3) |
Claim: There exists γ0>0 such that
m{x∈Ω; ˜a(x)|v0|q(x)≥γ0}≥γ0. | (3.4) |
Otherwise, we have
m{x∈Ω; ˜a(x)|v0|q(x)≥1n}=0, ∀n∈N. |
It follows that
0≤∫Ω˜a(x)|v0|q(x)+1dx<‖v0‖1n→0, as n→+∞. |
Hence v0=0, which contradicts ‖v0‖=1.
Set
Ω0={x∈Ω; ˜a(x)|v0|q(x)≥γ0}, Ωn={x∈Ω; ˜a(x)|vn|q(x)<1n} |
and
Ωcn={x∈Ω; ˜a(x)|vn|q(x)≥1n}. |
By (3.2) and (3.4), we obtain
m(Ωn∩Ω0)=m(Ω0∖(Ωcn∩Ω0))≥m(Ω0)−m(Ωcn∩Ω0)≥γ0−1n>γ02 |
for large enough n. Consequently, for all large n, we have
∫Ω˜a(x)|vn−v0|q(x)dx≥∫Ωn∩Ω0˜a(x)|vn−v0|q(x)dx≥12q+−1∫Ωn∩Ω0˜a(x)|v0|q(x)dx−∫Ωn∩Ω0˜a(x)|vn|q(x)dx≥(γ02q+−1−1n)m(Ωn∩Ω0)≥γ202q++1>0, |
which is a contradiction to (3.3). Therefore (3.1) holds. For the ϵ1 given in (3.1), let
Ωu={x∈Ω; ˜a(x)|u|q(x)≥ϵ1‖u‖q(x)}, ∀u∈F∖{0}. |
Then
m(Ωu)≥ϵ1 ∀ u∈F∖{0}. | (3.5) |
Using (B) and (3.5), for any u∈F∖{0} with ‖u‖≥1, we infer that
K(u)=∫Ω˜a(x)|u|q(x)dx≥∫Ωu˜a(x)|u|q(x)dx≥ϵ1‖u‖q−m(Ωu)≥ϵ21‖u‖q−. |
This shows that K(u)→∞ as ‖u‖→∞ on any finite dimensional subspace of X and this gives the proof of our desired result.
Lemma 3.4. Suppose that the conditions of Theorem 1.3 are satisfied. Then there exists a sequence ρk→0+ as k→+∞ such that
ak(λ)=infu∈Zk,‖u‖=ρkIλ(u)≥0, ∀k≥k1 |
and
dk(λ)=infu∈Zk,‖u‖≤ρkIλ(u)→0 as k→+∞ uniformly for λ∈[1,2]. |
Proof. By Propositions 1.2 and 2.1, we deduce that for any u∈Zk with ‖u‖<1, we have
Iλ(u)≥∫R2N∖(CΩ)2|u(x)−u(y)|p(x,y)2p(x,y)|x−y|N+sp(x,y)dxdy+∫Ω|u|¯p(x)¯p(x)dx+∫CΩβ(x)|u|¯p(x)v¯p(x)dx−λ∫Ωa(x)q(x)|u(x)|q(x)dx≥13p+−1p+‖u‖p+−λ‖u‖q+∫Ωa(x)q(x)(|u(x)|‖u‖)q(x)dx≥13p+−1p+‖u‖p+−2βkq−‖u‖q+. | (3.6) |
We denote ρk=(3p+−1(4p+)βkq−)1p+−q+. By Lemma 3.2 we deduce that ρk→0 as k→+∞. Then there exists k1∈N such that ρk≤13p+−1p+ for all k≥k1. Relation (3.6) implies that
ak(λ)=infu∈Zk,‖u‖=ρkIλ(u)≥12.3p+−1p+ρp++1k, for all k≥k1. |
Furthermore, by (3.6), we have
0≥infu∈Zk,‖u‖≤ρkIλ(u)≥−2βkq−‖u‖q−, ∀k≥k1. |
Since βk→0 as k→+∞, we deduce that
dk(λ)=infu∈Zk,‖u‖=ρkIλ(u)→0 as k→+∞ uniformly for λ∈[1.2]. |
This completes the proof.
Lemma 3.5. Assume that hypotheses of Theorem 1.3 are fulfilled. Then, for the sequence obtained in Lemma 3.4, there exists 0<rk<ρk for all k∈N such that
bk(λ)=maxu∈Yk,‖u‖=rkIλ(u)<0 for all λ∈[1,2]. |
Proof. Let u∈Yk with ‖u‖<1 and λ∈[1,2]. By (A), (P) and (3.1), there exists ϵk>0 such that
Iλ(u)=∫R2N∖(CΩ)2|u(x)−u(y)|p(x,y)2p(x,y)|x−y|N+sp(x,y)dxdy+∫Ω|u|¯p(x)¯p(x)dx+∫CΩβ(x)|u|¯p(x)v¯p(x)dx−λ∫Ωa(x)|u(x)|q(x)q(x)dx≤3p−‖u‖p−−ϵk‖u‖q−m(Ωu)≤3p−‖u‖p−−ϵ2k‖u‖q−. |
Since 0<q−<q+<p−<p+, we deduce that for small ‖u‖=rk we have
bk(λ)<0, ∀k∈N. |
This completes the proof of our lemma.
Proof of Theorem 1.3 completed. It is cleat that condition (T1) in Theorem 3.1 holds. Combining Lemmas 3.3, 3.4 and 3.5, we concludethat conditions (T2) and (T3) in Theorem 3.1 are satisfied. Then, by Theorem 3.1 there exist λn→1 and u(λn)∈Yn such that
I′λn|Yn(u(λn))=0, Iλn(u(λn))→ck∈[dk(2),bk(1)] |
as n→+∞.
For the sake of notational simplicity, we always set in what follows un=u(λn) for all n∈N.
Claim: the sequence (un) is bounded in X.
Otherwise, we can assume that (un) is unbounded in X. Without loss of generality, we can assume that ‖un‖>1 for all n≥1.
First, we can observe that there exists c>0 such that for large enough n,
⟨I′λn(un),un⟩≤‖un‖ and |Iλn(un)|≤c. | (3.7) |
Using relation (3.7), we have
c≥Iλn(un)≥12p+∫R2N∖(CΩ)2|un(x)−un(y)|p(x,y)|x−y|N+sp(x,y)dxdy+1p+∫Ω|un|¯p(x)dx+1p+∫CΩβ(x)|un|¯p(x)dx−1q−∫Ωa(x)|un(x)|q(x)dx. | (3.8) |
From Proposition 2.1, relation (3.8) and since q+<p−, we get that (un) is bounded in X. This proves that our claim is true. So, by Proposition 1.2 and up to a subsequence, we suppose that
un⇀u0 in X |
and
un→u0 in Lq(x)(Ω). |
In what follows we show that
un→u0 in X. |
Recalling that (un) is a bounded sequence, we get
limn→+∞⟨I′λn(un)−I′λn(u0),un−u0⟩=0. | (3.9) |
Hence, (3.9) and Proposition 1.2 give as n→+∞
o(1)=⟨I′λn(un)−I′λn(u0),un−u0⟩=∫R2N∖(CΩ)2|un(x)−un(y)|p(x,y)−2(un(x)−un(y))−|u(x)−u(y)|p(x,y)−2(u(x)−u(y))|x−y|N+sp(x,y)A(x,y)dxdy+∫Ω[|un|¯p(x)−2un−|u|¯p(x)−2u](un−u)dx+∫CΩβ(x)[|un|¯p(x)−2un−|u|¯p(x)−2u](un−u)dx |
where A(x,y)=(un(x)−u(x)−un(y)+u(y)).
We have for all n∈N
∫R2N∖(CΩ)2|un(x)−un(y)|p(x,y)−2(un(x)−un(y))−|u(x)−u(y)|p(x,y)−2(u(x)−u(y))|x−y|N+sp(x,y)A(x,y)dxdy≥0, |
∫Ω[|un|¯p(x)−2un−|u|¯p(x)−2u](un−u)dx≥0, |
and
∫CΩβ(x)[|un|¯p(x)−2un−|u|¯p(x)−2u](un−u)dx≥0 |
Therefore
limn→+∞∫R2N∖(CΩ)2|un(x)−un(y)|p(x,y)−2(un(x)−un(y))−|u(x)−u(y)|p(x,y)−2(u(x)−u(y))|x−y|N+sp(x,y)A(x,y)dxdy=0, | (3.10) |
limn→+∞∫Ω[|un|¯p(x)−2un−|u|¯p(x)−2u](un−u)dx=0, | (3.11) |
and
limn→+∞∫CΩβ(x)[|un|¯p(x)−2un−|u|¯p(x)−2u](un−u)dx=0. | (3.12) |
Let us now recall the Simon inequalities [28 formula 2.2]
{|x−y|p≤cp(|x|p−2x−|y|p−2y).(x−y)for p≥2|x−y|p≤Cp[(|x|p−2x−|y|p−2y).(x−y)]p2(|x|p+|y|p)2−p2for 1<p<2, | (3.13) |
for all x,y∈RN, where cp and Cp are positive constants depending only on p. Combining (3.10), (3.11), (3.12) and (3.13), we conclude that
limn→+∞‖un−u0‖=0. |
Now, by Theorem 3.1, we conclude the proof of Theorem 1.3.
The author declares no conflict of interest.
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