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Lions-type theorem of the p-Laplacian and applications

  • Yu Su and Zhaosheng Feng EMAIL logo
Published/Copyright: March 25, 2021

Abstract

In this article, our aim is to establish a generalized version of Lions-type theorem for the p-Laplacian. As an application of this theorem, we consider the existence of ground state solution for the quasilinear elliptic equation with the critical growth.

MSC 2010: 35A15; 35R11; 35J92

1 Introduction

Consider the quasilinear elliptic equation:

Δpu+V(|x|)|u|p2u=f(u),xRN, (𝓠)

where N ⩾ 3, p(1,N),V(|x|)=A|x|α,α(0,p), A > 0 is a real constant, and Δpu = div(|∇u|p–2u) is the p-Laplacian. Here, the nonlinearity f is given by

(F1) f(u) = |u|p*–2u + |u|q–2u + λ|u|pα2u , where λ>0,pα=p+p2αp(N1)α(p1),p=NpNp and qp(N+αp)Np,p.

Remark 1.1

The generalized version of the Berestycki-Lions conditions for the nonlinearity f is given as follows:

  1. fC(ℝ, ℝ), there exists C > 0 such that |sf(s)|C(|s|pα+|s|p) for s ∈ ℝ;

  2. lims0F(s)|s|pα=1andlims0F(s)|s|p=1, where F(s):=0sf(t)dt ; and

  3. there exists an s0 ∈ ℝ ∖ {0} such that F(s0) ≠ 0.

In view of (F1), clearly, the nonlinearity f satisfies the generalized version of the Berestycki-Lions conditions (F2)-(F4). This is thealmost optimalchoice of the nonlinearity f.

As is well known, for p = 2, equation (𝓠) is a model for describing the stationary state of reaction-diffusion equations in population dynamics [7]. It also arises in several other scientific fields such as plasma physics, condensed matter physics and cosmology [6]. The existence of solution of equation (𝓠) has been studied extensively by modern variational methods under various hypotheses on the singular potential V and the nonlinearity f. Let us briefly recall some related results. For p = 2 and V(|x|)=1|x|α, the existence and nonexistence of solutions to equation (𝓠) have been studied in [3, 4, 15, 17, 20, 23]. For p ≠ 2, the nonexistence results of equation (𝓠) were presented in [1, 5, 8, 9, 14, 16, 18] and the references therein.

For p ∈ (1, N) and V(x) = 1|x|p , Ghoussoub-Yuan [9] investigated the equation:

Δpuμ|x|p|u|p2u=|u|p2u,xRN, (1.1)

where N ⩾ 3, p ∈ (1, N) and μ0,Nppp, and established the existence of solutions to equation (1.1) by using the variational methods. Abdellaoui-Peral [1] considered the equation:

Δpuμ+k(x)|x|p|u|p2u=|u|p2u,xRN, (1.2)

and discussed the existence and nonexistence of solutions to equation (1.2) under different assumptions on k(x) by applying the concentration compactness principle and Pohožaev-type identity. Filippucci-Pucci-Robert [8] considered the problem:

Δpuμ|x|p|u|p2u=|u|p2u+|u|ps|x|s,xRN, (1.3)

where s ∈ (0, N) and ps=p(Ns)Np is the Hardy-Sobolev critical exponent, and obtained the existence results of equation (1.3) by the choice of a suitable energy level for the mountain pass theorem and analysis of concentration.

Su-Wang-Willem [18] dealt with a generalized version with the singular potential:

Δpu+V(|x|)|u|p2u=Q(x)f(u),xRN, (𝓖𝓠)

where 1 < p < N, and V and Q satisfy

  1. VC(0, ∞), V > 0 and there exist real numbers a and a0 such that

    lim infrV(r)ra>0andlim infr0V(r)ra0>0.
  2. QC(0, ∞), Q > 0 and there exist real numbers b and b0 such that

    lim suprQ(r)rb<andlim supr0Q(r)rb0<.

They attained the radial inequalities with respect to the parameters a, a0, b, b0, then established main results on continuous and compact embeddings and the existence of solution to equation (𝓖𝓠). Badiale-Guida-Rolando [5] generalized the embedding results under different conditions on V and Q, and explored the existence of solution to equation (𝓖𝓠) with the sub-critical and super-critical growth.

If a = a0 = -α and b = b0 = 0 in conditions (V1) and (Q1), equation (𝓖𝓠) reduces to (𝓠). Let us introduce the result on continuous and compact embeddings described in [18].

Proposition 1.1

Suppose that N ⩾ 3 and p ∈ (1, N). Then we have

Wrad1,p(RN,α)Lr(RN),r[pα,p],α(0,p),Wrad1,p(RN,α)Lr(RN),r[p,pα],α(p,N1p1p),Wrad1,p(RN,α)Lr(RN),r[p,),α[N1p1p,).

Furthermore, the embeddings are compact if r pα and rp*, where pα=p2(N1)+pαp(N1)α(p1)=p+p2αp(N1)α(p1),p=NpNp, and Wrad1,p(RN,α):=Drad1,p(RN)Lp(RN,α) is the set of radial functions in W1,p(ℝN, α).

It is very natural to ask whether there exists a solution to equation (𝓠) with the embedding top index p* and bottom index pα ? To the best of our knowledge, it seems that so far there is no affirmative answer in the literature.

From Proposition 1.1, the embeddings

Wrad1,p(RN,α)Lp(RN)andWrad1,p(RN,α)Lpα(RN)

are not compact. As a result, it is difficult to prove that the Palais-Smale (minimizing) sequence is strongly convergent if we seek solutions of equation (𝓠) with the critical exponent.

Lions [10] considered the noncompact embedding problem by the concentration-compactness principle: Only vanishing, dichotomy or tightness are possible. If one can exclude vanishing and dichotomy, then tightness occurs. It is not difficult to rule out vanishing. But sometimes it is hard to exclude the dichotomy. Therefore, it becomes interesting to ask under what conditions dichotomy cannot occur? In [11, pp. 232], Lions gave a useful answer.

Proposition 1.2

(Lions Theorem) Let N ⩾ 3 and p ∈ (1, N). Let {un} ⊂ W1,p(ℝN) be any bounded sequence satisfying

(Condition A) limnRN|un|rdx>0 for r ∈ (p, p*).

Then there exists {yn} ⊂ ℝN such that the sequence ūn(x) = un(x + yn) converges weakly and a.e. to ū ≢ 0 in Llocr (ℝN).

Following [10, 11], we can derive a similar result as follows immediately.

Proposition 1.3

(Lions-type theorem I) Let N ⩾ 3 and p ∈ (1, N). Let {un} ⊂ Wrad1,p (ℝN, α) be any bounded sequence satisfying

(Condition B) limnRN|un|rdx>0, where

r(pα,p)α(0,p),r(p,pα)α(p,N1p1p),r(p,)α[N1p1p,).

Then the sequence {un} converges weakly and a.e. to u ≢ 0 in Llocr (ℝN).

From Conditions A and B, we see that Propositions 1.2 and 1.3 provide a technical tool to the cases: (a) the nonlinearity f has neither the embedding top index nor embedding bottom index, and (b) the nonlinearity f has either the embedding top index or embedding bottom index. However, Propositions 1.2 and 1.3 become invalid when f contains both embedding top and bottom indices. Hence, we shall establish a more generalized result for α ∈ (0, p) as follows.

Theorem 1.1

Suppose that N ⩾ 3, p ∈ (1, N) and α ∈ (0, p). Let {un} ⊂ Wrad1,p (ℝN, α) be any bounded sequence satisfying

(Condition C) limnRN|un|pdx>0 and limnRN|un|pαdx>0.

Then the sequence {un} converges weakly and a.e. to u ≢ 0 in Llocp (ℝN).

Before presenting the existence of ground state solution to equation (𝓠), let us state the regularity properties of any nonnegative weak solutions of equation (𝓠) with α ∈ (0, p).

Theorem 1.2

Suppose that N ⩾ 3, p ∈ (1, N), α ∈ (0, p) and condition (F2) holds. If U is a nonnegative weak solution of equation (𝓠), then the following statements are true.

  1. ULr(ℝN) for r ∈ [ pα , ∞].

  2. U is a positive solution.

  3. U satisfies the Pohožaev-type identity:

    NppRN|U|pdx+NαpRNA|x|α|U|pdx=NRNF(U)dx.

As an application of Theorems 1.1 and 1.2, when the nonlinearity f satisfies condition (F1), i.e. equation (𝓠) takes the form

Δu+A|x|α|u|p2u=|u|p2u+|u|q2u+λ|u|pα2u,xRN, ( Spα )

we have

Theorem 1.3

Assume that N ⩾ 3, p ∈ (1, N ), α ∈ (0, p), q p(Np+α)Np,p and condition (F1) holds. Suppose that

αpSαpαpαpSppppαppλ>0,

where λ is a constant, Sα and S are the best constants of the following inequalities [2, 19]:

SαRN|u|pαdxppαuW1,p(RN,α)p,uWrad1,p(RN,α), (1.4)

and

SRN|u|pdxppuD1,p(RN)p,uD1,p(RN). (1.5)

Then equation ( Spα ) has a positive ground state solution u Wrad1,p (ℝN, α).

The rest of this paper is organized as follows. In Section 2, we briefly introduce some useful notations and inequalities. In Sections 3-5, we prove Theorems 1.1-1.3, respectively.

2 Preliminaries

For N ⩾ 3 and p ∈ (1, N), let

D1,p(RN):=uLp(RN)RN|u|pdx<

with the semi-norm

uD1,p(RN)p:=RN|u|pdx.

Let

W1,p(RN,α):=uD1,p(RN)uLp(RN,α)p=RNA|x|α|u|pdx<=D1,p(RN)Lp(RN,α)

with the norm

uW1,p(RN,α)p:=RN|u|pdx+RNA|x|α|u|pdx.

The following inequalities will play a crucial role in the proof of Theorem 1.3:

SαRN|u|pαdxppαuW1,p(RN,α)p,uWrad1,p(RN,α), (2.1)

and

SRN|u|pdxppuD1,p(RN)p,uD1,p(RN). (2.2)

A measurable function u : ℝN → ℝ belongs to the Morrey space with the norm ∥u𝓜q,ϖ(ℝN), where q ∈ [1, ∞) and ϖ ∈ (0, N], if and only if

uMq,ϖ(RN)q:=supR>0,xRNRϖNB(x,R)|u(y)|qdy<.

Lemma 2.1

([12], Refined Sobolev inequality with the Morrey norm) For N ⩾ 3 and p ∈ (1, N), there exists C > 0 such that for ι and ϑ satisfying ppι<1 and 1 ⩽ ϑ < p*, we have

RN|u|pdx1pCuD1,p(RN)ιuMϑ,ϑ(Np)p(RN)1ι,

for uD1,p(ℝN).

It follows from Lemma 2.1 and Wrad1,p (ℝN, α) ⊂ Drad1,p (ℝN) ⊂ D1,p(ℝN) that

RN|u|pdx1pCuW1,p(RN,α)ιuMϑ,ϑ(Np)p(RN)1ι,uWrad1,p(RN,α). (2.3)

To prove the generalized version of Lions-type theorem, we need the following technical lemma.

Lemma 2.2

([18]). Let N ⩾ 3, p ∈ (1, N) and α ∈ (0, p). Then the inequality

sup|x|>0|u(x)|C|x|p(N1)α(p1)p2uWrad1,p(RN,α)

holds for u Wrad1,p (ℝN, α).

Throughout this article, we will use the symbol C to denote a generic constant, possibly varying from line to line. However, special occurrences will be denoted by C1, or the like.

3 Proof of Theorem 1.1

In this section, by applying the refined Sobolev inequality with the Morrey norm and Lemma 2.2, we prove a generalized version of Lions-type theorem.

Proof of Theorem 1.1

We separate the proof into four steps.

  1. Note that {un} is a bounded sequence in Wrad1,p (ℝN, α). Then, up to a subsequence, we assume

    unuinWrad1,p(RN,α),unua.e.inRN,unuinLlocp(RN).

    According to (2.3) and Condition C, there exists a positive constant C such that for any n there holds

    unMp,Np(RN)C>0.

    On the other hand, from [12, pp 809] we note that {un} is bounded in Wrad1,p (ℝN, α) and

    Wrad1,p(RN,α)Drad1,p(RN)Lp(RN)Mp,Np(RN).

    Then we have

    unMp,Np(RN)C

    for some C > 0 independent of n. Hence, there exists a positive constant C0 such that for any n there holds

    C0unMp,Np(RN)C01.

    From this inequality, we deduce that for any n ∈ ℕ there exist σn > 0 and xn ∈ ℝN such that

    σnpB(xn,σn)|un(y)|pdyunMp,Np(RN)pC2nC1>0. (3.1)
  2. We show limn σn = σ̄ ≠ 0, where σ̄ ∈ (0, ∞).

    It suffices to show that limn σn ≠ ∞. Otherwise, we suppose limn σn = ∞. In view of the boundedness of {un} and Condition C, we get

    0<limnRN|un|pαdyC.

    Since N ⩾ 3, p ∈ (1, N) and α < p, we have

    p+N1ppα<0pα<p. (3.2)

    It follows from (3.1)-(3.2) that

    0<C1σnpB(xn,σn)|un(y)|pdyσnpB(0,σn)dypαppαB(xn,σn)|un(y)|pαdyppα=σnpωN1NσnNpαppαB(xn,σn)|un(y)|pαdyppασnp+N(1ppα)ωN1NpαppαRN|un(y)|pαdyppαCσnp+N(1ppα)0,asn,

    where ωN–1 is the volume of the unit sphere in ℝN. This is a contradiction.

    By the Bolzano-Weierstrass theorem, up to a subsequence, still denoted by {σn}, there exists σ̄ ∈ [0, ∞) such that

    limnσn=σ¯.

    We now show limn σn = σ̄ ≠ 0. Suppose on the contrary that limn σn = σ̄ = 0. By using the uniform boundedness of {un} in Wrad1,p (ℝN, α), we have

    ClimnRN|un|pdypplimnunWrad1,p(RN,α)pC¯.

    It follows from Hölder’s and Sobolev’s inequalities that

    B(0,σn)|un|pαdyB(0,σn)dyppαpB(0,σn)|un|pdypαpSpαpB(0,σn)dyppαpRN|un|pdypαppB(0,σn)|un|pdyCSpαpB(0,σn)dyppαpB(0,σn)|un|pdy.

    Similarly, for each z ∈ ℝN we have

    B(z,σn)|un|pαdyCSpαpB(0,σn)dyppαpB(z,σn)|un|pdy.

    Covering ℝN by balls of radius σn, in such a way that each point of ℝN is contained in at most N + 1 balls, we find

    RN|un|pαdyC(N+1)SpαpB(0,σn)dyppαpRN|un|pdyC(N+1)SpαpB(0,σn)dyppαp=C(N+1)SpαpωN1N1pαpσnN(1pαp),

    where ωN–1 is the volume of the unit sphere in ℝN.

    Taking n → ∞ and applying limn σn = 0 leads to

    limnRN|un|pαdyC(N+1)SpαpωN1N1pαplimnσnN(1pαp)=0,

    which yields a contradiction to limn N |un|p* dx > 0 given in Condition C.

    Using limn σn = σ̄ ≠ 0, up to a subsequence, we have σn(σ¯2,2σ¯) and

    2pσ¯pB(xn,σn)|un(y)|pdyC1>0,

    which gives

    B(xn,σn)|un(y)|2dyC1σ¯p2p>0. (3.3)
  3. We show that {xn} is a bounded sequence.

    By way of contradiction, we can assume |xn| → ∞ as n → ∞. According to Lemma 2.2, we have

    sup|x|>0|un(x)|C|x|p(N1)α(p1)p2unWrad1,p(RN,α)C|x|p(N1)α(p1)p2.

    For any C1σ¯p2p|B(0,2σ¯)|1p>ε>0, there exists an M > 0 such that for any n > M there holds

    |un(x)|C||xn|σn|p(N1)α(p1)p2ε,xBc(0,||xn|σn|).

    From B(xn, σn) ⊂ Bc(0, ||xn| – σn|), it follows that

    B(xn,σn)|un(y)|pdyεpB(xn,σn)dy=εp|B(xn,σn)|=εp|B(0,σn)|εp|B(0,2σ¯)|<C1σ¯p2p.
  4. Note that {xn} is bounded. There exists 0 < < ∞ such that 0 ⩽ |xn| < . In view of limn σn = σ̄ ≠ 0, up to a subsequence, we have

    B(xn,σn)B(0,|xn|+σn)B(0,C~+2σ¯).

    From (3.1), we deduce that

    0<C1σ¯p=C1limnσnplimnσnplimnσnpB(xn,σn)|un|pdy=limnB(xn,σn)|un|pdylimnB(0,C~+2σ¯)|un|pdy.

    Applying the embedding Wrad1,p (ℝN, α) ↪ Drad1,p (ℝN) ↪ Llocp (ℝN), we obtain u ≢ 0.□

4 Proof of Theorem 1.2

In this section, we prove that any nonnegative weak solutions of equation (𝓠) with α ∈ (0, p) have additional regularity properties.

Lemma 4.1

Assume that all the conditions described in Theorem 1.2 hold. For each L > 2, define

UL(x)=U(x)ifU(x)L,LifU(x)>L.

Set ŪL = UULp(μ1) , where μ > 1. Let t be the best embedding constant from Wrad1,p (ℝN, α) to Lt(ℝN) for t ∈ [ pα , p*]. Then we have

RN|UULμ1|tdxptCμpC~tRNUpαp|UULμ1|pdx+RNUpp|UULμ1|pdx. (4.1)

Proof

Let U be a nonnegative ground state solution of equation (𝓠). We show that ŪL Wrad1,p (ℝN, α). By a straightforward calculation, we get

RN|(UULp(μ1))|pdx=RN|ULp(μ1)U+p(μ1)UULp(μ1)1UL|pdx2pRN|ULp(μ1)|p|U|pdx+(2p)p(μ1)pRN|UULp(μ1)1|p|UL|pdx=2pRN|ULp(μ1)|p|U|pdx+(2p)p(μ1)p{x|U(x)L}|ULp(μ1)|p|U|pdx2pLp2(μ1)(1+(μ1)p)RN|U|pdx,

and

RNA|x|α|UULp(μ1)|pdxLp2(μ1)RNA|x|α|U|pdx.

This implies that ŪL Wrad1,p (ℝN, α).

Note that U is a nonnegative ground state solution of equation (𝓠). Then

RN|U|p2Uφdx+RNA|x|α|U|p2Uφdx=RNf(U)φdx.

Substituting ŪL into the above equation, we get

RN|U|p2UU¯Ldx+RNA|x|α|UULμ1|pdx=RNf(U)U¯Ldx. (4.2)

Since

RNUULp(μ1)1|U|p2UULdx={x|U(x)L}Up(μ1)|U|pdx0,

it follows that

RN|U|p2UU¯Ldx=RNULp(μ1)|U|pdx+p(μ1)RNUULp(μ1)1|U|p2UULdxRNULp(μ1)|U|pdx. (4.3)

Note that

RN|(UULμ1)|pdx[2p+(2p)p(μ1)p]RNULp(μ1)|U|pdx(2p)pμpRNULp(μ1)|U|pdx. (4.4)

It follows from (4.2)-(4.4) and Proposition 1.1 that

C~tRN|UULμ1|tdxpt(2p)pμpRN|U|p2UU¯Ldx+RNA|x|α|UULμ1|pdxCμpRNUpp|UULμ1|pdx+RNUpαp|UULμ1|pdx.

We are now ready to prove Theorem 1.2.

Proof of Theorem 1.2

We divide the proof into three parts.

Part (i). We first show the L estimate of U by the following four steps.

  1. We claim that

    1+RN|U|pμ1dxpp(μ11)<,

    where μ1:=1+ppαp.

    Taking ∈ ℝ+ and using Hölder’s inequality, we can derive

    RNUpp|UULμ1|pdxd¯ppα{x|U(x)d¯}Upαp|UULμ1|pdx+{x|U(x)>d¯}Upp|UULμ1|pdxd¯ppαRN|U|pα+pμpdx+{x|U(x)>d¯}UpdxpppRN|UULμ1|pdxpp.

    We choose such that

    {x|U(x)>d¯}UpdxpppC~p2Cμp.

    Substituting the above two inequalities into (4.1) with the choice of t = p*, we get

    RN|UULμ1|pdxpp2CμpC~pRNUpαp|UULμ1|pdx+d¯ppαRN|U|pα+pμpdx.

    Taking the limit as L → ∞ in the above inequality leads to

    RN|U|pμdxpp2CμpC~p1+d¯ppαRN|U|pα+pμpdx.

    Let pα + p ∈ ( pα , p*] and choose μ(1,1+ppαp]. Then

    ULpμ(RN).

    Hence, we have

    ULpˇ1(RN),pˇ1[pα,p]p,p1+ppαp.

    We now choose μ1 := 1 + ppαp . Then we obtain p*μ1 p,p1+ppαp and

    1+RN|U|pμ1dxpp(μ11)<.
  2. We show that

    1+RN|U|pμ2dxpp(μ21)(Cμ2)pμ211+RN|U|pμ1dxpp(μ11),

    where μ2 – 1 = ( pp )(μ1 – 1).

    Let μ2 := 1 + pp ⋅ (μ1 – 1). Then p* + 2p = p*μ1 and μ2 – 1 = ( pp )(μ1 – 1). Let μ ∈ [μ1, μ2]. We find

    pα<pα+pμp<p+pμppμ1.

    From Lemma 4.1, we get

    RN|U|pμdxppCμpC~pRN|U|pα+pμpdx+RN|U|p+pμpdx<.

    For each μ ∈ [μ1, μ2], we have ULp*μ(ℝN) and

    ULpˇ2(RN),pˇ2[pα,pμ1][pμ1,pμ2].

    Set μ = μ2. Then

    RN|U|pμ2dxppCμ2pC~pRN|U|pα+pμ2pdx+RN|U|p+pμ2pdx<.

    Let a2=p(ppα)p(μ21) and b2 = pα + 2pa2. Then pb2pa2=p+pμ2p. It follows from Young’s inequality that

    RN|U|pα+pμ2pdx=RN|U|a2|U|b2dxa2pRN|U|pdx+pa2pRN|U|p+pμ2pdxC1+RN|U|p+pμ2pdx.

    Thus, we deduce

    RN|U|pμ2dxppCμ2p1+RN|U|p+pμ2pdx.

    For every x1, x2 > 0, we know that

    (x1+x2)ppx1pp+x2pp.

    We then obtain

    1+RN|U|pμ2dxpp1+RN|U|pμ2dxppCμ2p1+RN|U|p+pμ2pdx.

    That is,

    1+RN|U|pμ2dxpp(μ21)(Cμ2)pμ211+RN|U|pμ1dx1μ21=(Cμ2)pμ211+RN|U|pμ1dxpp(μ11).
  3. We show that

    1+RN|U|pμ3dxpp(μ31)(Cμ3)pμ311+RN|U|pμ2dxpp(μ21),

    where μ3 – 1 = ( pp )(μ2 – 1).

    Let μ3 := 1 + pp ⋅ (μ2 – 1). Then p* + 3p = p*μ2 and μ3 – 1 = ( pp )(μ2 – 1). Let μ ∈ [μ2, μ3]. Then

    pα<pα+pμp<p+pμppμ2.

    So we get

    RN|U|pμdxppCμpC~pRN|U|pα+pμpdx+RN|U|p+pμpdx<.

    For each μ ∈ [μ2, μ3], we have ULp*μ(ℝN) and

    ULpˇ3(RN),pˇ3[pα,pμ2][pμ2,pμ3].

    Set μ = μ3. Then

    RN|U|pμ3dxppCμ3pC~pRN|U|pα+pμ3pdx+RN|U|p+pμ3pdx<.

    Let a3=p(ppα)p(μ31) and b3 = pα + 3pa3. Then pb3pa3=p+pμ3p. It follows from Young’s inequality that

    RN|U|pα+pμ3pdxC1+RN|U|p+pμ3pdx.

    Hence, we obtain

    1+RN|U|pμ3dxpp(μ31)(Cμ3)pμ311+RN|U|pμ2dxpp(μ21).
  4. Iterating the above process and recalling that

    p+pμi+1p=pμi,i1andiN,

    we have

    μi+11=ppi(μ11)

    and

    1+RN|U|pμi+1dxpp(μi+11)(Cμi+1)pμi+111+RN|U|pμidx1μi+11=(Cμi+1)pμi+111+RN|U|pμidxpp(μi1).

    For m ∈ ℕ, we further get

    i=1m(Cμi+1)pμi+111+RN|U|pμ1dxpp(μ11)1+RN|U|pμm+1dxpp(μm+11)RN|U|pμm+1dxpp(μm+11).

    If ∫N |U|p*μm+1 dx ⩽ 1, then

    i=1m(Cμi+1)pμi+111+RN|U|pμ1dxpp(μ11)RN|U|pμm+1dxp+p2ppαpμm+1=ULpμm+1(RN)p+p2ppα.

    That is,

    ULpμm+1(RN)i=1m(Cμi+1)1μi+111+RN|U|pμ1dx1p(μ11)ppαppα+p. (4.5)

    If ∫N |U|p*μm+1 dx > 1, then

    i=1m(Cμi+1)pμi+111+RN|U|pμ1dxpp(μ11)RN|U|pμm+1dxppμm+1=ULpμm+1(RN)p.

    That is,

    ULpμm+1(RN)i=1m(Cμi+1)1μi+111+RN|U|pμ1dx1p(μ11). (4.6)

    Note that

    limmi=1m(Cμi+1)pμi+11=limmepi=1mlnCμi+11+lnμi+1μi+11.

    For the series i=1lnCμi+11 , using the root test, we get

    limilnCμi+11i=limilnC(pp)i(μ11)i=pp<1,

    which indicates i=1lnCμi+11 < ∞.

    For the series i=1lnμi+1μi+11 , by using the ratio test, we find

    limilnμi+2μi+21μi+11lnμi+1=pplimiln1+pp(μi+11)lnμi+1pplimilnpp+pp(μi+11)lnμi+1=pplimilnpplnμi+1+lnμi+1lnμi+1<1,

    which implies i=1lnμi+1μi+11 < ∞. Hence, we have i=1(Cμi+1)pμi+11<.

    Letting m → ∞ in (4.4) and (4.5), we obtain

    UL(RN)<.

    Part (ii). We rewrite equation (𝓠) as –ΔpU = g(x, U), where

    g(x,U)=A|x|αU+f(U).

    For all Ω ⊂ ⊂ ℝN ∖ {0}, there exists C(Ω) > 0 such that |g(x, U)| ⩽ C(Ω) (1 + |U|p*–1) for xΩ. It follows from Theorem 1.2 (i) and [21, Theorem 1 and Proposition 1] that UC1(ℝN ∖ {0}). Finally, the strict positivity follows form the strong maximum principle [22].

    Part (iii). Applying Theorem 1.2 (ii) and following [8, Claim 5.3], we can derive the Pohožaev-type identity

    NppRN|U|pdx+NαpRNA|x|α|U|pdx=NRNF(U)dx.

    Consequently, the proof is completed.□

5 Proof of Theorem 1.3

As we see, equation ( Spα ) is variational and its solutions are the critical points of the functional defined in Wrad1,p (ℝN, α) by

J(u):=1puWrad1,p(RN,α)pλpαRN|u|pαdx1qRN|u|qdx1pRN|u|pdx.

From Proposition 1.1, we know that JC1( Wrad1,p (ℝN, α), ℝ). It is easy to see that if u Wrad1,p (ℝN, α) is a critical point of J, i.e.

0=J(u),φ=RN(|u|p2uφ+A|x|α|u|p2uφ)dxλRN|u|pα2uφdxRN|u|q2uφdxRN|u|p2uφdx

for all φ Wrad1,p (ℝN, α), then u is a weak solution of equation ( Spα ).

Define

c=infγΓsupt[0,1]J(γ(t))>0,

where

Γ=γC[0,1],Wrad1,p(RN,α)|γ(0)=0,J(γ(1))<0.

Define

N={uWrad1,p(RN,α)|J(u),u=0,u0},

and let

c¯=infuNJ(u).

It is easy to check that c=c¯=c¯¯:=infuWrad1,p(RN,α){0}supt0J(tu)>0.

Lemma 5.1

Assume that all the conditions described in Theorem 1.3 hold. Then

0<c<c:=minαNp1λppαpSαpαpαp,1NSppp.

Proof

If αpSαpαpαpSppppαppλ>0, then

αNp1λppαpSαpαpαp1NSppp.

We choose

ωσ(x)=CσNpp(p1)(σpp1+|x|pp1)Npp

and

wσD1,p(RN)p=w1D1,p(RN)p=RN|w1|pdx=RN|wσ|pdx=Sppp.

A straightforward calculation gives

RN|wσ|p|x|αdxCRN1|x|ασNp(σpp1+|x|pp1)NpdxC01ρα1(σpp1+ρpp1)NpρN1dρ=C01ρN1α(1+ρpp1)Npdρ+C1ρN1α(σpp1+ρpp1)NpdρC01ρN1α(σpp1+ρpp1)Npdρ+C1ρN1αp(Np)p1dρ.

It is not difficult to see that

01ρN1α(σpp1+ρpp1)Npdρ01ρN1α(σpp1)Npdρ<.

In view of p ∈ (1, N ), we have N – 1 – α p(Np)p1 < –1 and

1ρN1αp(Np)p1dρ<.

This implies that wσ Wrad1,p (ℝN, α). So we have

RN|wσ|pαdx=σppα(Np)p(N1)α(p1)RN|w1|pαdx,RN|wσ|qdx=σq+(pq)NpRN|w1|qdx,RN1|x|α|wσ|pdx=σpαRN1|x|α|w1|pdx,

and limt J(twσ) = –∞.

Let σ > tσ > 0 satisfy

supt0J(twσ)=J(tσwσ)andJ(t¯σwσ)<0.

Taking γ(t) = tt̄σwσ, we get

cmaxt[0,1]J(γ(t))=J(tσwσ).

Note that

0=ddt|t=tσJ(twσ)=tσp1tσp1w1D1,p(RN)p+σpαtσp1RNA|x|α|w1|pdxλσppα(Np)p(N1)α(p1)tσpα1RN|w1|pαdxσq+(pq)Nptσq1RN|w1|qdx. (5.1)

Let t0 := lim supσ0 tσ. We claim that t0 < ∞. Otherwise, we assume that t0 = ∞. Taking an upper limit as σ → 0 in (5.1), we get

lim supσ0tσp1w1D1,p(RN)p+σpαtσp1RNA|x|α|w1|pdx=lim supσ0tσp1w1D1,p(RN)p+λσppα(Np)p(N1)α(p1)tσpα1RN|w1|pαdx+σq+(pq)Nptσq1RN|w1|qdx. (5.2)

It follows from p < p* and lim supσ0 tσ = ∞ that

lim supσ0tσp1w1D1,p(RN)p+σpαRNA|x|α|w1|pdx<lim supσ0tσp1w1D1,p(RN)plim supσ0tσp1w1D1,p(RN)p+λσppα(Np)p(N1)α(p1)tσpα1RN|w1|pαdx+σq+(pq)Nptσq1RN|w1|qdx.

This contradicts (5.2). That is, t0 < ∞.

Passing to an upper limit as σ → 0 in (5.1) leads to

0=t0p1t0p1w1D1,p(RN)p,

which implies

t0p1t0p1=0andt0=1.

Let {σn} be a sequence such that σ → 0 as n → ∞. Then, up to a subsequence, still defined by {σn}, we have

t02<tσn. (5.3)

Hence, we can choose σ̃ > 0 small enough such that

t02<tσ~t0.

Set

g(t)=tpptppandg(t)=tp1tp1.

Then, we have g′(t0) = 0, g′(t) < 0 for t > t0, and g′(t) > 0 for t < t0. Hence, g(t) attains its maximum at t0. That is,

g(t)<g(t0)=1N (5.4)

for any tt0.

It follows from q > p(N+αp)Np and (5.3)-(5.4) that

J(tσ~wσ~)tσ~pptσ~ppw1D1,p(RN)p+σ~pαtσ~RNA|x|α|w1|pdxσ~q+(pq)Nptσ~qqRN|w1|qdxtσ~pptσ~ppw1D1,p(RN)p=tσ~pptσ~ppSppp<1NSppp

for sufficiently small σ̃. Consequently, we arrive at the desired result.□

5.1 Perturbation Equation

Applying Theorems 1.1 and 1.2, it is easy to prove the existence of positive ground state solution of the following equation (with small ε > 0, see [18]):

Δpu+A|x|α|u|p2u=|u|pε2u+|u|q2u+λ|u|pα+ε2u,xRN. ( Spα+ε )

Set the energy functional of equation ( Spα+ε ) as follows:

Jε(u):=1pRN(|u|p+A|x|α|u|p)dx1qRN|u|qdx1pεRN|u|pεdxλpα+εRN|u|pα+εdx.

Let vε be a positive ground state solution of equation ( Spα+ε ). For all φ Wrad1,p (ℝN, α), it follows that

0=Jε(vε),φ=RN(|vε|p2vεφ+A|x|α|vε|p2vεφ)dxRN|vε|q2vεφdxRN|vε|pε2vεφdxλRN|vε|pα+ε2vεφdx,
0=Pε(vε)=1pRN|vε|pdx+NαpNRNA|vε|p|x|αdx1qRN|vε|qdx1pεRN|vε|pεdxλpα+εRN|vε|pα+εdx,

and

cε=Jε(vε)=1pRN(|vε|p+A|x|α|vε|p)dx1qRN|vε|qdx1pεRN|vε|pεdxλpα+εRN|vε|pα+εdx.

We then have the following lemma for equation ( Spα+ε ).

Lemma 5.2

Assume that all the conditions described in Theorem 1.3 hold. Then the following statements are true.

  1. For each u Wrad1,p (ℝN, α) ∖ {0}, there exists a unique τε > 0 such that Pε(uτε) = 0 for ε ∈ (0, ε0], where

    uτ(x)=u(xτ),τ>0,0,τ=0.

    Moreover, we have Jε(uτε) = maxτ0 Jε(uτ).

  2. cε = cεP for ε ∈ (0, ε0], where

    cε=inf{Jε(u)|uWrad1,p(RN,α)andJε(u)=0},

    and

    cεP=inf{Jε(u)|uWrad1,p(RN,α)andPε(u)=0}.
  3. lim supε0 cεc.

  4. cε ⩾ 0 for ε ∈ [0, ε0].

  5. Let εn → 0+ and {vεn} ⊂ Wrad1,p (ℝN, α) satisfy

    Jεn(vεn)=cεn,Pεn(vεn)=0,Jεn(vεn)=0.

Then, {vεn} is bounded in Wrad1,p (ℝN, α) and lim infn cεn > 0.

Proof

  1. For each u Wrad1,p (ℝN, α) ∖ {0}, we set

    φε(τ)=Jε(uτ)=τNppRN|u|pdx+τNαpRNA|u|p|x|αdxτNqRN|u|qdxλτNpα+εRN|u|pα+εdxτNpεRN|u|pεdx.

    A direct calculation gives

    φε(τ)=NppτNp1RN|u|pdx+NαpτNα1RNA|u|p|x|αdxNτN1qRN|u|qdxλNτN1pα+εRN|u|pα+εdxNτN1pεRN|u|pεdx.

    In view of N ⩾ 3, p ∈ (1, N ) and α ∈ (0, p), we find that φε (τ) > 0 for small τ > 0 and limτφε(τ)<0. Then there exists τε > 0 such that φε (τε) = 0 and Jε(uτε) = maxτ0 Jε(uτ). Moreover, Pε(uτε)=1Nτεφε(τε)=0.

  2. On one hand, Theorem 1.2 implies that cε cεP for ε ∈ [0, ε0]. On the other hand, we have

    cε=cεmp:=infγΓsupt[0,1]Jε(γ(t))>0,

    where

    Γ=γC[0,1],Wrad1,p(RN,α)|γ(0)=0,Jε(γ(1))<0.

    It is easy to see that there exists τ1 large enough such that Jε(uτ1) < 0. Hence, we can choose γ(t) = u1.

    Using Lemma 5.2 (i), we have cεmpmaxτ0Jε(uτ)=Jε(uτε). Since u is arbitrary, we obtain cεmpcεP and cε = cεP for ε ∈ (0, ε0].

  3. For any δ ∈ (0, 12 ), there exists u Wrad1,p (ℝN, α) ∖ {0} with P(u) = 0 such that J(u) < c + δ. In view of P(u) = 0, we get

    NppRN|u|pdx+NαpRNA|u|p|x|αdx=NqRN|u|qdx+λNpαRN|u|pαdx+NpRN|u|pdx>0.

    Then there exists τ̄ > 0 large enough such that

    J(uτ¯)=τ¯NppRN|u|pdx+τ¯NαpRNA|u|p|x|αdxτ¯NqRN|u|qdxτ¯NλpαRN|u|pαdx+1pRN|u|pdx1.

    We now show the continuity of τNpα+εRN|u|pα+εdx and τNpεRN|u|pεdx on (τ, ε) ∈ [0, τ̄] × (0, ε0).

    Firstly, it is easy to check the continuity of τNpα+ε and τNpε on (τ, ε) ∈ [0, τ̄] × (0, ε0).

    Secondly, let 0 < ε1 < ε2 < ε0. Then pα + ε1 < pα + ε2 < p*. It follows from Hölder’s and Young’s inequalities that

    RN|u|pα+ε2dxppαε2ppαε1RN|u|pα+ε1dx+ε2ε1ppαε1RN|u|pdx,

    which gives

    RN|u|pα+ε2dxRN|u|pα+ε1dxε1ε2ppαε1RN|u|pα+ε1dx+ε2ε1ppαε1RN|u|pdx.

    That is,

    RN|u|pα+ε2dxRN|u|pα+ε1dxε1ε2ppαε1RN|u|pα+ε1dxRN|u|pdx. (5.5)

    From (5.5), it is not difficult to see the continuity of ∫N |u|pα+ε dx on ε ∈ (0, ε0). Similarly, we can prove the continuity of ∫N |u|p*ε dx on ε ∈ (0, ε0) too.

    Thirdly, let f1(τ,ε)=τNpα+ε,f2(τ,ε)=τNpε,g1(ε)=RN|u|pα+εdx and g2(ε) = ∫N |u|p*ε dx. Then f1(τ, ε) ⋅ g1(ε) and f2(τ, ε) ⋅ g2(ε) are continuous on (τ, ε) ∈ [0, τ̄] × (0, ε0).

    Finally, by using the continuity of τNpα+εRN|u|pα+εdx and τNpεRN|u|pεdx on (τ, ε) ∈ [0, τ̄] × (0, ε0), there exists ε̄ > 0 such that for all ε ∈ (0, ε̄) and τ ∈ [0, τ̄] there holds

    |Jε(uτ)J(uτ)|=τNλpα+εRN|u|pα+εdxλpαRN|u|pαdx+1pεRN|u|pεdx1pRN|u|pdxτNλpα+εRN|u|pα+εdxλpαRN|u|pαdx+τN1pεRN|u|pεdx1pRN|u|pdx<δ,

    which implies

    Jε(uτ¯)12,ε(0,ε¯).

    Note that Jε(uτ) > 0 for τ small enough. Then there exists τ̄ε ∈ (0, τ̄) such that ddτJε(uτ)|τ=τ¯ε, and Pε(uτ̄ε) = 0. By Lemma 5.2 (i), we know J(uτ̄ε) ⩽ J(u). Thus, for any ε ∈ (0, ε̄) there holds

    cεJε(uτ¯ε)J(uτ¯ε)+δJ(u)+δ<c+2δ.

    Hence, lim supε0 cεc.

  4. By a direct calculation, we have

    cε=Jε(vε)Pε(vε)=1NRN|vε|2dx+αpNRNA|vε|2|x|αdx0.
  5. By virtue of Lemma 5.2 (iii), we have

    c+1cεn=Jεn(vεn)Pεn(vεn)=1NRN|vεn|pdx+αpNRNA|vεn|p|x|αdxCvεnWrad1,p(RN,α)p.

    Namely, {vεn} is bounded in Wrad1,p (ℝN, α).

    It follows from (2.1)-(2.2) that

    0=Pεn(vεn)CvεnWrad1,p(RN,α)pCvεnWrad1,p(RN,α)qCvεnWrad1,p(RN,α)pα+εnCvεnWrad1,p(RN,α)pεn,

    which implies that there exists C > 0 independent of n such that

    vεnWrad1,p(RN,α)C.

    Hence, we obtain lim infn cεn > 0.□

5.2 Ground State Solution

In this subsection, by using the perturbation method [13] and Pohožaev-type identity [1], we present the proof of Theorem 1.3.

Proof of Theorem 1.3

We separate our proof into two steps.

  1. We take ε → 0 in equation ( Spα+ε ). For each small εn, there exists a positive ground state solution vεn. Using Lemma 5.2 (iii), we have

    c+1cεn=Jεn(vεn)1pα+εnJεn(vεn),vεn1p1pα+εnvεnWrad1,p(RN,α)p.

    This implies that {vεn} is bounded in Wrad1,p (ℝN, α). Then, up to a subsequence, we assume that

    vεnvinWrad1,p(RN,α),vεnva.e.inRN,vεnvinLr(RN),r(pα,p).

    For any φ Wrad1,p (ℝN, α), as n → ∞, we claim that

    RN|vεn|pεn2vεnφdx=RN|v|p2vφdx+o(1) (5.6)

    and

    RN|vεn|pα+εn2vεnφdx=RN|v|pα2vφdx+o(1). (5.7)

    Here, we only show (5.6), because the proof of (5.7) can be processed in a similar manner. For any ϵ > 0, there exists a sufficiently large R > 0 such that

    |x|>R|vεn|pεn2vεnφdx|x|>R|v|p2vφdx|x|>R|vεn|pεn1|φ|dx+|x|>R|v|p1|φ|dx|x|>R|vεn|pεndx11pεn|x|>R|φ|pεndx1pεn+|x|>R|v|pdx11p|x|>R|φ|pdx1p<ϵ2.

    On the other hand, note that {vεn} is bounded in Wrad1,p (ℝN, α). There exists C > 0 such that

    |x|R|vεn|pεndx11pεn<C.

    In view of E ⊂ ℝN and small εn > 0, it follows from Holder’s and Young’s inequalities that

    E|φ|pεndxE|φ|pαdxεnppαE|φ|pdxppαεnppαεnppαE|φ|pαdx+ppαεnppαE|φ|pdxE|φ|pαdx+E|φ|pdx.

    For any ϵ > 0, there exists δ > 0 such that when E ⊂ {x ∈ ℝN ||x| ⩽ R} with |E| < δ there holds

    E|vεn|pεn2vεnφdxE|vεn|pεndx11pεnE|φ|pεndx1pεnE|vεn|pεndx11pεnE|φ|pαdx+E|φ|pdx1pεn<Cϵ,

    where the last inequality is true due to the absolute continuity of E|φ|pαdx and ∫E |φ|p* dx.

    Making use of the fact |vεn|p*εn–2 vεnφ → |v|p*–2 a.e. in ℝN, by Vitali’s convergence Theorem, we have

    |x|R|vεn|pεn2vεnφdx=|x|R|v|p2vφdx+ϵ2.

    Then

    RN|vεn|pεn2vεnφdxRN|v|p2vφdx|x|>R|vεn|pεn2vεnφdx|x|>R|v|p2vφdx+|x|R|vεn|pεn2vεnφdx|x|R|v|p2vφdxϵ.

    Hence, we arrive at (5.6).

    It follows from (5.6) and (5.7) that

    0=Jεn(vεn),φ=RN(|vεn|p2vεnφ+A|x|α|vεn|p2vεnφ)dxRN|vεn|q2vεnφdxRN|vεn|pεn2vεnφdxλRN|vεn|pα+εn2vεnφdx=RN(|v|p2vφ+A|x|α|v|p2vφ)dxRN|v|q2vφdxRN|v|p2vφdxλRN|v|pα2vφdx=J(v),φ.

    This indicates that v is a weak solution of equation (𝓠).

  2. We claim that v ≢ 0.

    In view of Jεn(vεn),vεn=0, we get

    RN|vεn|pdx+RNA|vεn|p|x|αdx=RN|vεn|qdx+RN|vεn|pεndx+λRN|vεn|pα+εndx. (5.8)

    It follows from Holder’s and Young’s inequalities that

    RN|vεn|pα+εndxRN|vεn|pαdxppαεnppαRN|vεn|pdxεnppαppαεnppαRN|vεn|pαdx+εnppαRN|vεn|pdx, (5.9)

    and

    RN|vεn|pεndxRN|vεn|pαdxεnppαRN|vεn|pdxppαεnppαεnppαRN|vεn|pαdx+ppαεnppαRN|vεn|pdx. (5.10)

    Substituting (5.9) and (5.10) into (5.8) leads to

    RN|vεn|pdx+RNA|vεn|p|x|αdx1+εn(λ1)ppαRN|vεn|pdx+λ+εn(1λ)ppαRN|vεn|pαdx+RN|vεn|qdx. (5.11)

    It suffices to show that there exists C > 0 such that CvεnWrad1,p(RN,α). Otherwise, we assume that vεnWrad1,p(RN,α)0. Then it yields cεn → 0, which contradicts lim infn cεn > 0, see Lemma 5.2 (v).

    It follows from (5.11) and 0<CvεnWrad1,p(RN,α) that only one of the following statements is true.

    (i)RN|vεn|pαdx0andCRN|vεn|pdx;or(ii)CRN|vεn|pαdxandRN|vεn|pdx0;or(iii)CRN|vεn|pαdxandCRN|vεn|pdx. (5.12)

    We first exclude (i) in (5.12). Suppose on the contrary that (5.12) (i) holds. It follows from (5.12) (i) and (5.11) that

    RN|vεn|pdxRN|vεn|pdx+RNA|vεn|p|x|αdxRN|vεn|pdxSppRN|vεn|pdxpp,

    which gives

    SpppRN|vεn|pdx.

    In view of Lemma 5.2, we get

    ccεn=Jεn(vεn)1NPεn(vεn)=1NRN|vεn|2dx+αpNRNA|vεn|p|x|αdx1NRN|vεn|pdx1NSppp.

    This yields a contradiction with the fact of c<min1NSppp,αpN1λppαpSαpαpαp, see Lemma 5.1. Hence, (5.12) (i) can not occur.

    We now exclude (ii) in (5.12). Suppose on the contrary that (5.12) (ii) holds. It follows form (5.12) (ii) and (5.11) that

    RN|vεn|pdx+RNA|vεn|p|x|αdxλRN|vεn|pαdxλSαpαpRN|vεn|pdx+RNA|vεn|p|x|αdxpαp,

    which gives

    1λppαpSαpαpαpRN|vεn|pdx+RNA|vεn|p|x|αdx.

    Using Lemma 5.2 yields

    ccεn=Jεn(vεn)Pεn(vεn)=1NRN|vεn|pdx+αpNRNA|vεn|p|x|αdxαpNRN|vεn|pdx+RNA|vεn|p|x|αdxαpN1λppαpSαpαpαp.

    This contradicts the fact of c<min1NSppp,αpN1λppαpSαpαpαp, see Lemma 5.1. Hence, (5.12) (ii) can not occur either.

    We now draw a conclusion that (5.12) (iii) is true. By virtue of Theorem 1.1, we have v ≢ 0. In view of Theorem 1.2, P(v) = 0 and the weakly lower semi-continuity of the norm, we obtain

    cJ(v)=J(v)P(v)=1NRN|v|pdx+αpNRNA|v|p|x|αdxlim infn1NRN|vεn|pdx+lim infnαpNRNA|vεn|p|x|αdx=Jεn(vεn)1NPεn(vεn)=cεnc.

    Consequently, v is a positive ground state solution.□


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Acknowledgement

This work is supported by Postdoctoral Science Foundation (2020M671835).

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Received: 2020-11-02
Accepted: 2021-01-07
Published Online: 2021-03-25

© 2021 Yu Su and Zhaosheng Feng, published by De Gruyter

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

Articles in the same Issue

  1. Editorial
  2. Editorial to Volume 10 of ANA
  3. Regular Articles
  4. Convergence Results for Elliptic Variational-Hemivariational Inequalities
  5. Weak and stationary solutions to a Cahn–Hilliard–Brinkman model with singular potentials and source terms
  6. Single peaked traveling wave solutions to a generalized μ-Novikov Equation
  7. Constant sign and nodal solutions for superlinear (p, q)–equations with indefinite potential and a concave boundary term
  8. On isolated singularities of Kirchhoff equations
  9. On the existence of periodic oscillations for pendulum-type equations
  10. Multiplicity of concentrating solutions for a class of magnetic Schrödinger-Poisson type equation
  11. Nehari-type ground state solutions for a Choquard equation with doubly critical exponents
  12. Gradient estimate of a variable power for nonlinear elliptic equations with Orlicz growth
  13. The structure of 𝓐-free measures revisited
  14. Solvability of an infinite system of integral equations on the real half-axis
  15. Positive Solutions for Resonant (p, q)-equations with convection
  16. Concentration behavior of semiclassical solutions for Hamiltonian elliptic system
  17. Global existence and finite time blowup for a nonlocal semilinear pseudo-parabolic equation
  18. On variational nonlinear equations with monotone operators
  19. Existence results for nonlinear degenerate elliptic equations with lower order terms
  20. Blow-up criteria and instability of normalized standing waves for the fractional Schrödinger-Choquard equation
  21. Ground states and multiple solutions for Hamiltonian elliptic system with gradient term
  22. Positivity of solutions to the Cauchy problem for linear and semilinear biharmonic heat equations
  23. Convex solutions of Monge-Ampère equations and systems: Existence, uniqueness and asymptotic behavior
  24. Multiple solutions for critical Choquard-Kirchhoff type equations
  25. Regularity for sub-elliptic systems with VMO-coefficients in the Heisenberg group: the sub-quadratic structure case
  26. Inducing strong convergence of trajectories in dynamical systems associated to monotone inclusions with composite structure
  27. A posteriori analysis of the spectral element discretization of a non linear heat equation
  28. Liouville property of fractional Lane-Emden equation in general unbounded domain
  29. Large data existence theory for three-dimensional unsteady flows of rate-type viscoelastic fluids with stress diffusion
  30. On some classes of generalized Schrödinger equations
  31. Variational formulations of steady rotational equatorial waves
  32. On a class of critical elliptic systems in ℝ4
  33. Exponential stability of the nonlinear Schrödinger equation with locally distributed damping on compact Riemannian manifold
  34. On a degenerate hyperbolic problem for the 3-D steady full Euler equations with axial-symmetry
  35. Existence, multiplicity and nonexistence results for Kirchhoff type equations
  36. Combined effects of Choquard and singular nonlinearities in fractional Kirchhoff problems
  37. Convergence analysis for double phase obstacle problems with multivalued convection term
  38. Multiple solutions for weighted Kirchhoff equations involving critical Hardy-Sobolev exponent
  39. Boundary value problems associated with singular strongly nonlinear equations with functional terms
  40. Global solvability in a three-dimensional Keller-Segel-Stokes system involving arbitrary superlinear logistic degradation
  41. Multiplicity and concentration behaviour of solutions for a fractional Choquard equation with critical growth
  42. Concentration results for a magnetic Schrödinger-Poisson system with critical growth
  43. Periodic solutions for a differential inclusion problem involving the p(t)-Laplacian
  44. The concentration-compactness principles for Ws,p(·,·)(ℝN) and application
  45. Regularity for commutators of the local multilinear fractional maximal operators
  46. An improvement to the John-Nirenberg inequality for functions in critical Sobolev spaces
  47. Local versus nonlocal elliptic equations: short-long range field interactions
  48. Analysis of a diffusive host-pathogen model with standard incidence and distinct dispersal rates
  49. Blowing-up solutions of the time-fractional dispersive equations
  50. Fixed point of some Markov operator of Frobenius-Perron type generated by a random family of point-transformations in ℝd
  51. Non-stationary Navier–Stokes equations in 2D power cusp domain
  52. Non-stationary Navier–Stokes equations in 2D power cusp domain
  53. Nontrivial solutions to the p-harmonic equation with nonlinearity asymptotic to |t|p–2t at infinity
  54. Iterative methods for monotone nonexpansive mappings in uniformly convex spaces
  55. Optimality of Serrin type extension criteria to the Navier-Stokes equations
  56. Fractional Hardy-Sobolev equations with nonhomogeneous terms
  57. New class of sixth-order nonhomogeneous p(x)-Kirchhoff problems with sign-changing weight functions
  58. On the set of positive solutions for resonant Robin (p, q)-equations
  59. Solving Composite Fixed Point Problems with Block Updates
  60. Lions-type theorem of the p-Laplacian and applications
  61. Half-space Gaussian symmetrization: applications to semilinear elliptic problems
  62. Positive radial symmetric solutions for a class of elliptic problems with critical exponent and -1 growth
  63. Global well-posedness of the full compressible Hall-MHD equations
  64. Σ-Shaped Bifurcation Curves
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  66. On singular quasilinear elliptic equations with data measures
  67. On the sub–diffusion fractional initial value problem with time variable order
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  69. Ground state solutions for a class of fractional Schrodinger-Poisson system with critical growth and vanishing potentials
  70. Initial boundary value problems for the three-dimensional compressible elastic Navier-Stokes-Poisson equations
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