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www.elsevier.com/locate/anihpc

Existence, non-existence and regularity of radial ground states for p-Laplacian equations with singular weights

Patrizia Pucci

, Raffaella Servadei

Dipartimento di Matematica e Informatica, Università degli Studi di Perugia, Via Vanvitelli 1, 06123 Perugia, Italy Received 12 September 2006; accepted 14 February 2007

Available online 17 July 2007

Abstract

By the Mountain Pass Theorem and the constrained minimization method existence of positive or compactly supported radial ground states for quasilinear singular elliptic equations with weights are established. The paper also includes the discussion of regularity and the validity of useful qualitative properties of the solutions, which seems of independent interest. Finally, a Pohozaev type identity is produced to deduce some non-existence results.

©2007 Elsevier Masson SAS. All rights reserved.

MSC:primary 35J15; secondary 35J70

Keywords:Quasilinear singular elliptic equations with weights

1. Introduction

Existence and non-existence, as well as qualitative properties, of non-trivial non-negative solutions for elliptic equations with singular coefficients were recently studied by several authors, e.g., in bounded domains and forp=2 cf. [2,10,12,18,23,42], and for generalp >1 see [17,20,24,50]; while in unbounded domains and forp=2 cf. [27, 31,42,47], and for generalp >1 see [1,11,14,21,25,36,45]. There is a large literature onp-Laplacian equations in the entireRn, but the nonlinear structure, objectives and methods differ somehow from those presented here.

More precisely, we consider the following quasilinear singular elliptic equation puλ|u|p2u+μ|x|α|u|q2u+h

|x|

f (u)=0 inRn\ {0},

λ, μ∈R, 1< p < n, (1.1)

wherep=div(|Du|p2Du),Du=(∂u/∂x1, . . . , ∂u/∂xn)and either 0α < pq < pα=p(nα)/(np)or α=q=p (=pα); whileh:R+→R+andf:R→Rare given continuous functions.

Homogeneous Dirichlet problems associated to equations of type (1.1) are studied by Ekeland and Ghoussoub in [17] and by Ghoussoub and Yuan in [24] in smooth bounded domains ofRn containing zero, whenλ=0,h≡1,

This research was supported by the ProjectMetodi Variazionali ed Equazioni Differenziali Non Lineari.

* Corresponding author.

E-mail addresses:[email protected] (P. Pucci), [email protected] (R. Servadei).

0294-1449/$ – see front matter ©2007 Elsevier Masson SAS. All rights reserved.

doi:10.1016/j.anihpc.2007.02.004

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f (u)=c|u|s2uwithc >0 andps < p=pn/(np). They give existence and multiplicity results of non-trivial non-negative solutions by means of variational methods and of the Hardy–Sobolev inequality (see, e.g., [2,12,20,34]), when either 0α < pq < pα orα=q=p (=pα).

In this paper we extend the existence results of [17,24] to the entireRn, and to the case in whichλ >0,his a general non-trivial weight such thath(|x|)=o(|x|β)as|x| →0, withβ∈ [0, p), bounded at infinity, see Section 2, whilef is possibly different from a pure power. In particular, in Theorem 3.1 we prove the existence of a radial ground state of (1.1), i.e. a non-trivial non-negative weak solution which tends to zero at infinity, by the celebrated Mountain Pass Theorem of Ambrosetti and Rabinowitz and the Hardy–Sobolev inequality, whenf is of the canonical form required in [3] and with uf (u) >0 for u=0. Then, using the regularity results of [41], and an application of the strong maximum principle due to Vázquez [48] (see also [38,39]), we show that the constructed ground stateuis of class C1(Rn\ {0})and by Proposition 3.2 also of classC(Rn), provided that 0max{α, β}< pand sopositive everywhere inRn. As a consequence of Theorems 2.1 and 2.2 of [41], we also show that the solutionugiven by Theorem 3.1 is in Lmloc(Rn)for anym∈ [1,∞)if 0α < pq < pα, while, if 0max{α, β}< p, thenuL(Rn). Moreover, as an application of [41, Theorem 2.5], we prove thatuHloc2,p(Rn\ {0})when 1< p2 anduHloc2,p(Rn)if furthermore 0max{α, β}p−1.

Since in the degenerate casep >2 the uniform ellipticity ofpis lost at zeros ofDu, the best we can expect, even in the standard no weighted case of (1.1), is to have solutions of classCloc1,θ(Rn\ {0})(see [16]). Of course, for (1.1) much less could be expected and regularity was an open problem. A partial result is given in Proposition 3.2 for radial ground states of (1.1), provided they are assumed a prioribounded. However Proposition 3.2 applies to the solution constructed in Theorem 3.1 when 0max{α, β}< p. Also this result seems to the authors new.

In Section 4 we prove a Pohozaev type identity which yields some non-existence statements for (1.1). The main non-existence Theorems 4.10 and 4.11 for (1.1) extend several previous results, see e.g. [20, Lemma 3.7] established in bounded star-shaped domains, whenλ=β=0 and [24, Theorem 2.1] stated forλ=0,q=pα,α∈ [0, p],h≡1 andf (u)=c|u|p2u,c >0. In particular, as a consequence of Theorems 4.10 and 4.11 we obtain a non-existence result for thedoubly criticalequation

puλ|u|p2u+μ|x|p|u|p2u+γ|x|β|u|pβ2u=0 a.e. inRn,

λ=0, γ , μ∈R, β < p, pβ=p(nβ)/(np), (1.2)

which extends, e.g., [33, Theorem 1.3] given forp=2 andλ=β=0.

Moreover, we show that

pu+γ|x|β|u|s2u=0 inΩ, γ∈R, s >1, (1.3)

whereΩ=Rn whenβ0, whileΩ=Rn\ {0}whenβ(0, p), admits only the trivial solution whenever either γ 0, or γ >0 ands=pβ. This result, when the regular periodic function of [47] is zero, extends [47, Theo- rem 0.1(ii)] proved by Terracini in the case p=2 andβ=0. Therefore, in Section 5 we give the explicit positive radial ground state for (1.3) only in the remaining possible case, that is whens=pβ,β < pandγ >0, defined by

u(x)=c

1+ |x|(pβ)/(p1)(np)/(pβ)

, c= nβ

γ

np p−1

p1(np)/p(pβ)

. (1.4)

This includes the standard solution for the no weighted case β =0, p=2 and s=2 (see, e.g., [28,44,49] and references therein), as well as the ground state found for (1.3) when 0β < pands=pβ in [17,24] for allp >1, and in [10,27] forp=2. Clearly the solutionugiven in (1.4) is of classD1,p(Rn)L(Rn)C(Rn)C(Rn\{0}), while is of classH1,p(Rn)if and only ifn > p2. The regularity of (1.4) atx=0 is presented in Table 2 below.

In Section 6 we use a different approach for studying (1.1) whenλ=μ=0,h(r)=rβ, butβ < pis possibly negative. More precisely, we consider

pu+ |x|βf (u)=0 inΩ, β < p, (1.5)

whereΩ is defined as above, in the so callednormal case(see [35]), that is whenf is a general continuous function which is negative near the origin and positive at infinity. Roughly speaking, f (u)∼= −c|u|q1 as u→0+, with q >1, c >0, and limu→∞u1pβf (u)=0, withpβ=p(nβ)/(np). After the papers of [4,5] related to elliptic problems with the Laplace operator in the normal case, equations involving thep-Laplacian operator inRn, were

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Table 1

1< p2 p >2

β <1 C2(Rn) C1(Rn)

1β < p C0,(ploc β)/(p1)(Rn)

Table 2

1< p2 p >2

β <2p C2(Rn)

β=2p C2(Rn) Cloc1,1(Rn)

2p < β <1 C2(Rn) Cloc1,(1β)/(p1)(Rn) 1β < p C0,(ploc β)/(p1)(Rn)

treated largely in literature (see e.g. [13,19,22] for the no weighted case, that is whenβ=0 in (1.5), and [11] for general weighted equations).

In Propositions 6.1 and 6.2, we give some qualitative properties of bounded radial ground states of class C1(Rn\ {0})of (1.5) and discuss their regularity, using the theory of singular elliptic problems with general weights developed in [36].

In Theorem 6.7, adapting the constrained minimization method of Coleman, Glaser and Martin [15], we prove the existence of aboundedcontinuous radial ground stateu of (1.5) in the entireRn. It is anopen problemif any radial ground state of (1.5) is bounded inRn, that is nearx =0. Theorem 6.7 extends to the weighted caseβ < p the existence results obtained forβ=0 by Berestycki and Lions in [4] whenp=2, and by Citti in [13] for general p >1; and also Theorems 7 and 10 of [11] given for div(g(|x|)|Du|p2Du)+h(|x|)f (u)=0 in the special case in whichg≡1,h(r)=rβ,β < p, andf is continuous also atu=0. Finally, we observe that in this paper no locally Lipschitz continuity is assumed onf as required in [11] and in several previous papers in the no weighted case (see e.g. [14,19,22,36] and the papers quoted there).

Moreover, when 1< p2, as a consequence of [41, Theorem 2.5], we show that the ground stateu given in Theorem 6.7 is of classHloc2,p(Rn\ {0})anduHloc2,p(Rn), if furthermoreβ < n/p.

While the ground states of (1.1) and (1.3) are necessarily positive inRn, for (1.5) they are compactly supported when 1< q < pand positive when qp, where q represents as above the growth off near zero, see condition (F5). Moreover, when 1< q < p, the ground stateuconstructed in Theorem 6.7 has the further regularity described in Table 1 (see Proposition 6.1). On the other hand, whenqp, thenuhas the further regularity described in Table 2 (see Proposition 6.2).

Table 2 extends to the general nonlinear weighted equation(1.5)in the normal case the regularity established for (1.3)whens=pβ,γ >0and the explicit ground state(1.4)is known. Furthermore both tables improve the regularity results given by Citti in Remarks 1.2 and 1.3 of [13] for the no weighted caseβ=0. It remains anopen problemif any solution of (1.5) is radially symmetric with respect tox=0.

In Theorem 6.9 we present an application of Theorem 6.7 and Lemma 4.6 to the case when the nonlinearity in (1.5) is of polynomial type. Theorem 6.9 extends to the weightedp-Laplacian case the existence and non-existence results given by Berestycki and Lions in [4, Example 2] in the no weighted Laplacian caseβ=0 andp=2.

The main results of this paper and of [41] were presented in a unified way, but without proofs, in the survey [40].

2. Preliminaries

Here some preliminary results are presented as well as embedding theorems of the Sobolev spaces H1,p(Rn), Hrad1,p(Rn) andD1,p(Rn)into weighted Lebesgue spaces related to (1.1), proved by means of the Hardy–Sobolev inequality (see, e.g., [2,12,20,34]) and the Caffarelli–Kohn–Nirenberg inequality [9]. For other results of this type see, e.g., [2,12,50] and references therein.

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Throughout the paper we assume that 1< p < n. In the sequelH1,p(Rn)denotes the usual Sobolev space, endowed with the normu =(upp+ Dupp)1/p, andD1,p(Rn)is the closure ofC01(Rn)with respect to the normDup. Letα∈Rand consider also the weighted Lebesgue space

Lpα Rn

=Lp

Rn,|x|αdx

=

uL1loc Rn

:

Rn

u(x)p|x|αdx <

,

endowed with the norm up,α=(

Rn|u(x)|p|x|αdx)1/p. Note that Lpα(Rn) is a reflexive Banach space and Lpα(Rn)is its dual space (see Theorem 5.3 in [30]), where 1/p+1/p=1.

By the Hardy–Sobolev inequality (cf. Lemma 2.1 of [20]) we have that upp,p=

Rn

u(x)p|x|pdxCn,pp

Rn

Du(x)pdx=Cn,pp Dupp (2.1)

for anyuD1,p(Rn), and so in particular up,pCn,pu for alluH1,p

Rn . Actually, the best Hardy–Sobolev constant (see [20]) is

inf

D1,p(Rn)\{0}

Dup

up,p =Cn,p1, Cn,p= p np.

In the following we adopt the notationBR= {x∈Rn: |x|R},ΩR=Rn\BR,R >0.

Forβ∈R, let us introduce, for general weightsw, the functional space Wβ=

wLR)for anyR >0: w=0, w0 a.e. inRnand lim

|x|→0|x|βw(x)=0

, and Lsw(Rn)=Ls(Rn, w(x) dx)= {uL1loc(Rn):

Rn|u(x)|sw(x) dx <∞}, endowed with the norm us,w= (

Rn|u(x)|sw(x) dx)1/s, when 1s <∞.

LetcT denote the best constant of the Sobolev embeddingD1,p(Rn) Lp(Rn), that is cT =cT(n, p)=π1/2n1/p

p−1 np

1/p

(1+n/2)(n) (n/p)(1+nn/p)

1/n

, see [46], and put forwWβ andR >0

CHS=CHS(n, p, β, s, w)=cn(sT p)/psmax

Cn,pβ/s,w1/sLR)

. (2.2)

Lemma 2.1.

(i) Let0β < pand letwWβ. Then, the embeddingH1,p(Rn) Lsw(Rn)is continuous for alls∈ [p, pβ], where

pβ=pnβ

np. (2.3)

(ii) Ifβ=p, then the embeddingH1,p(Rn) Lpw(Rn)is continuous for allwWp. Moreover in both cases(i)and(ii)for alluH1,p(Rn)

us,wCHSu, (2.4)

whereCHSis given in(2.2), withR=R(w)so small that0w(x)|x|β for allxBR\ {0}. (iii) For the standard weightw(x)= |x|β∈ [0, p], cases(i)and(ii)trivially apply, with

CHS=CHS(n, p, β, s)=cn(sT p)/psCn,pβ/s. (2.5)

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Proof. (i) Since wWβ, there exists R >0 depending on w such that w(x)|x|β for 0<|x|R. For any uHrad1,p(Rn), by the properties ofwand H˝older’s inequality,

uss,w=

BR

u(x)sw(x) dx+

ΩR

u(x)sw(x) dx

BR

u(x)β|x|βu(x)sβdx+ wLR) ΩR

u(x)sdx

BR

u(x)p|x|pdx

β/p

BR

|u(x)|qdx

(pβ)/p

+ wLR)uss

uβp,pusqβ+ wLR)uss, (2.6)

whereq=p(sβ)/(pβ). Now, for anyt∈ [p, p], setting εt=p(pt )

t (pp)∈ [0,1], we have for alluH1,p(Rn)

utuεptu1pεt c1Tεtuεtu1εt =c1Tεtu, (2.7) by the interpolation inequality and the Sobolev embedding theorem. Since s ∈ [p, pβ] ⊂ [p, p] and so also q∈ [p, p], by (2.6), (2.7), and the Hardy–Sobolev inequality (2.1), it follows that

uss,wc(1Tεq)(sβ)Cβn,pDuβpusβ+c(1Tεs)swLR)us cn(sT p)/p

Cn,pβ + wLR)

us

CHSus

,

that is (2.4) holds. Hence,H1,p(Rn)is continuously embedded inLsw(Rn)for alls∈ [p, pβ].

(ii) Fixε(0,1] and letδ=δ(ε)such thatw(x)ε|x|p for all x, with 0<|x|δ. By the Hardy–Sobolev inequality we easily obtain, as in the proof of part (i) ,

upp,wε

Bδ

u(x)p|x|pdx+ wLδ) Ωδ

u(x)pdxεCn,pp Dupp+ wLδ)upp, which yields (2.4) whenε=1 andR=δ(1). Hence,H1,p(Rn)is continuously embedded inLpw(Rn).

(iii) If β=0, the assertion is the standard Sobolev embedding H1,p(Rn) Ls(Rn)for all s∈ [p, p]. For β(0, p) we can repeat the proof of part (i) withR=(np)/p=1/Cn,p. Whenβ =p, case (iii) is a trivial consequence of (2.1). 2

The next result is a particular case of the Caffarelli–Kohn–Nirenberg inequality (see [9]).

Lemma 2.2.Letα∈ [0, p]. Then, the embeddingD1,p(Rn) Lpαα(Rn)is continuous, wherepα=p(nα)/(np) and in turn alsoH1,p(Rn) Lpαα(Rn)is continuous.

When α=p, Lemma 2.2 reduces to the Hardy–Sobolev inequality. Of course in Hrad1,p(Rn), i.e. the space of functionsuH1,p(Rn)which are radial, much more can be said.

Lemma 2.3.

(i) Let0β < pand letwWβ. Then, the embeddingHrad1,p(Rn) Lsw(Rn)is continuous for alls∈ [p, pβ]and compact for alls∈ [p, pβ), wherepβis given in(2.3).

(ii) Ifβ=p, then the embeddingHrad1,p(Rn) Lpw(Rn)is compact for allwWp.

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Proof. (i) The continuity of the embeddingHrad1,p(Rn) Lsw(Rn)follows by Lemma 2.1.

Now, let(uk)kbe a bounded sequence inHrad1,p(Rn). Thus, there existsuHrad1,p(Rn)such that, up to a subsequence, uk uweakly inHrad1,p(Rn)ask→ ∞. SinceHrad1,p(Rn)is compactly embedded inLs(Rn)for alls∈ [p, p), we have that

Duk Du inLp Rn

and uku inLs Rn

(2.8) ask→ ∞. Arguing as in (2.6), fors∈ [p, pβ)we have

ukuss,wCn,pβ DukDuβpukusqβ+ wLR)ukuss

KCn,pβ ukusqβ+ wLR)ukuss, (2.9) whereq=p(sβ)/(pβ)and for some positive constantKby virtue of (2.8). Sinceq < pbecauses∈ [p, pβ), the assertion follows from (2.8) and (2.9).

(ii) The continuity of the embedding Hrad1,p(Rn) Lpw(Rn)follows by Lemma 2.1. Let(uk)k be a bounded se- quence inHrad1,p(Rn). Up to a subsequence, still denoted by(uk)k, we have thatuk uinHrad1,p(Rn)andukuin Lp(Rn)ask→ ∞. As above

ukupp,wεCpn,pDukDupp+ wLδ)ukupp. (2.10) SinceHrad1,p(Rn)is compactly embedded inLp(Rn), then (2.10) implies that

lim sup

k

ukupp,wεCn,pp sup

k

DukDupp=Const.ε, and the assertion follows at once sinceε >0 is arbitrary. 2

Remark 2.4. If w(x)= |x|α, with α∈ [0, p), then the embedding Hrad1,p(Rn) Lpα(Rn) is compact. Indeed, for α=0, the assertion is trivial, while forα(0, p) it follows from Lemma 2.3(i) . Forα=p the embedding Hrad1,p(Rn) Lpp(Rn)is continuous by Hardy–Sobolev inequality (2.1).

Lemma 2.1 can be refined when H1,p(Rn)is replaced by H01,p(Ω), whereΩ is any bounded open set ofRn. Indeed in this case the embedding H01,p(Ω) Lsw(Ω) is continuous for alls∈ [1+β/p, pβ]and compact for alls∈ [1+β/p, pβ),β∈ [0, p). The proof of the continuity is similar to that of Lemma 2.1 since in the bounded case (2.7) holds for allt ∈ [1, p], and q∈ [1, p]if s∈ [1+β/p, pβ]. For the compactness we can argue as in Lemma 2.3, sinceH01,p(Ω)is compactly embedded inLs(Ω)for alls∈ [1, p). Whenβ=0 the result reduces to the usual Sobolev theorem (see [7]); however 1+β/p< pfor allβ∈ [0, p).

Now we present some preliminary results which will be useful in the sequel. The first lemma, stated here for the weighted spacesLsw(Rn), is well-known in the usual Lebesgue spaces (see, for instance, Theorem IV.9 of [7]). The proof is left to the reader, since it is standard.

Lemma 2.5.Let1s <and letwWβ. If(uk)k is a sequence inLsw(Rn)anduLsw(Rn)such thatukuin Lsw(Rn), then there exist a subsequence(ukj)jof(uk)kand a functionϕLsw(Rn)such that a.e. inRn

(i)ukju asj→ ∞; (ii)ukj(x)ϕ(x) for allj ∈N.

In this paper we need also the following lemma, which is a corollary of Theorem 1 of Brézis and Lieb [8].

Lemma 2.6.Let1s <∞, let(uk)k be a sequence inLs(Rn)and letuLs(Rn). Ifuk uinLs(Rn)anduku a.e. onRnask→ ∞, then

limk

ukssukuss

= uss.

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We recall that whens >1 and(uk)kconverges a.e. inRntou, thenuk uinLs(Rn)if and only if supkuks<∞ (see Theorem 13.44 of [26]).

A result similar to Lemma 2.6 continues to hold, essentially with the same proof, in the weighted Lebesgue space Lss(Rn)=Ls(Rn,|x|sdx).

Lemma 2.7.Let1s <, let(uk)kbe a sequence inLss(Rn)and letuLss(Rn). Ifuk uinLss(Rn)anduku a.e. inRnask→ ∞, then

limk

ukss,sukuss,s

= uss,s.

Even if Boccardo and Murat in [6] treat only the case of bounded domains Ω of Rn, the almost everywhere convergence of the gradients together with Remarks 2.1 and 2.2 of [6] continues to hold whenΩ is replaced byRn. In particular, as a consequence of Theorem 2.1 of [6], we have the following lemma.

Lemma 2.8.Let(uk)k be a sequence in H1,p(Rn)and uH1,p(Rn)such thatuk uinH1,p(Rn),uku in Lp(Rn)and a.e. inRn ask→ ∞. Let(gk)k be a bounded sequence inL1loc(Rn). Assume finally that eachuk is a weak solution of

puk=gk inRn.

ThenDukDua.e. inRnask→ ∞.

The next lemma is essentially due to Strauss in [43] and is useful to prove the main Theorems 3.1 and 6.7. Let Drad1,p(Rn)denote the space of radial functionsuD1,p(Rn).

Lemma 2.9.

(i) LetuHrad1,p(Rn). Then for allR >0we have, a.e. inRn, u(x)

[(p−1)/(n−p)]1/pωn1/pDup|x|(np)/p, if0<|x|R, [max{p−1,1}]1/pωn1/pu · |x|(n1)/p, if|x|> R,

where ωn is the measure of the unit sphere of Rn. Moreover, |x|(n1)/pu(x)→ 0 as |x| → ∞ and uC0,1/p(Rn\BR).

(ii) IfuD1,prad(Rn), then u(x)

(p−1)/(n−p)1/p

ωn1/pDup|x|(np)/p a.e. inRn,

|x|(np)/pu(x)→0as|x| → ∞and againuC0,1/p(Rn\BR)for anyR >0.

Proof. (i) It is enough to prove this part foruC0,rad1 (Rn), sinceC0,rad1 (Rn)is dense inHrad1,p(Rn). Letρ > r >0.

By using H˝older’s inequality we have that u(ρ)−u(r)

ρ

r

u(t )dt ρ

r

|u(t )|ptn1dt

1/p ρ r

t(n1)/(p1)dt 1/p

p−1

np 1/p

ωn1/pDupρ(np)/(p1)r(np)/(p1)1/p.

Passing to the limit as ρ → ∞ and taking into account that 1< p < n, it follows that |u(x)| [(p −1)/

(np)]1/pωn1/pDup|x|(np)/pa.e. inRn. In particular, the first inequality of part (i) holds.

Now, letr >0. By the Young inequality we get

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u(r)pp

r

u(t )p1u(t )dtpr(n1)

r

u(t )p1u(t )tn1dt r(n1)

(p−1)

r

u(t )ptn1dt+

r

u(t )ptn1dt

max{p−1,1}r(n1)

r

u(t )ptn1dt+

r

u(t )ptn1dt

,

and in turn|x|(n1)/pu(x)→0 as|x| → ∞. Moreover|u(x)|[max{p−1,1}]1/pωn1/pu · |x|(n1)/pa.e. inRn. Finally, forρ > rR >0, again by H˝older’s inequality

u(ρ)u(r)

ρ

r

u(t )dt(ρr)1/p ρ

r

u(t )pdt 1/p

r(n1)/p ρ

r

u(t )ptn1dt 1/p

r)1/p ωn1/pR(n1)/pDupr)1/p,

which completes the proof of (i) .

(ii) For the second part of the lemma we can argue as above. 2

Throughout the paper by aground stateof (1.1) we mean a non-trivial non-negative weak solution of (1.1) which tends to zero as|x| → ∞. While by afast decaysolution of (1.1) we mean a non-trivial weak solutionuof (1.1) such that

|xlim|→∞|x|(np)/(p1)u(x) exists and is finite.

3. An existence theorem

In this section we prove the existence of a positive radial ground state of (1.1), when the function f :R+0 →R satisfies the following conditions

(F1) f is continuous inR+0;

(F2) there exista0,b >0andp < ssuch that|f (u)|aup1+bus1inR+0; (F3) limu0+upF (u)=0,whereF (u)=u

0 f (v) dvfor allu∈R+0; (F4) 0< sF (u)uf (u)for allu∈R+.

Clearlyf (0)=0 by (F1) and (F2). The standard prototype forf, verifying (F1), (F2), withuf (u) >0 foru=0, as required in (F4), is given byf (u)=a|u|p2u+b|u|s2u, witha0,b >0. Of course condition (F4) fails when s > p. Indeed, foru=0 we have exactly the reverse inequalitysF (u)uf (u)=a(sp)|u|p/p0. Therefore these nonlinearities do not verify the structure (F1)–(F4).

The power functionf (u)=b|u|s2uorf (u)=b|u|s1arctanu, both withb >0, satisfy (F1)–(F4) whens > p.

By (F1)–(F3) it follows that for anyε >0 there existsCε>0 such that

F (u)ε|u|p+Cε|u|s (3.1) for any u∈R+0. Clearly, whena=0 in (F1), then (3.1) holds also forε=0, withCε=b/s. Condition (F4) easily yields that there existU >0 and a positive constantdsuch that

F (u)d|u|s for alluwithuU. (3.2)

For the weight functionh:R+→R+in (1.1) we assume condition

(9)

(H1) h=h(|x|)Wβ for someβ∈ [0, p).

Now we give an existence result for (1.1) by means of the Mountain Pass Theorem of [3].

Theorem 3.1.Assume(F1)–(F4)and(H1). Consider(1.1), with 0β < p < s < pβ, λ >0, 0μpCqHS< qmin{1, λ},

and either 0α < pq < pα or α=q=p(=pα), (3.3)

whereCHS=CHS(n, p, α, q)is the constant of the embeddingHrad1,p(Rn) Lqα(Rn)given in(2.5). Then(1.1),(3.3) admits a radial ground stateuHrad1,p(Rn). Moreover,

(i) uCloc1,θ(Rn\ {0})for someθ(0,1);

(ii) |Du|p2DuC1(Rn\ {0});

(iii) uis positive, solves Eq.(1.1),(3.3)pointwise inRn\ {0},x, Du(x)<0for allxwith|x|sufficiently large and

|Du(x)| →0as|x| → ∞;

(iv) uis a fast decay solution of (1.1),(3.3);

(v) if0α < pq < pα, thenuLmloc(Rn)for anym∈ [1,∞);

(vi) if0max{α, β}< p, thenuL(Rn);

(vii) if1< p2, thenuHloc2,p(Rn\ {0});if furthermore0max{α, β}p−1, thenuHloc2,p(Rn).

Proof. Since we are interested in positive solutions of (1.1), we extendf in the entireRasf (u)=0 foru <0.

First of all suppose 0α < pq < pα. By Lemma 2.3 and (F2) the functional J(u)= 1

p

Dupp+λupp

μ

quqq,α

Rn

F u(x)

h

|x| dx

is well-defined inHrad1,p(Rn). By Lemma 2.1(iii) we have q

Dupp+λupp

μpuqq,α

qmin{1, λ} −μpCHSq uqp

up. (3.4)

Letδ(0,1]. Then for anyuHrad1,p(Rn)withu =δwe get

qmin{1, λ} −μpCHSq uqpqmin{1, λ} −μpCHSq :=γpq >0 by assumption. Hence, from (3.4),

J(u)γup

Rn

F u(x)

h

|x| dx.

By (3.1) for everyε >0 there is a positive constantCεsuch that J(u)γupεupp,hCεuss,h

γεC1

upCεC2us, (3.5)

whereC1=max{Cn,pβ ,hLR)}andC2=cn(sT p)/pC1 and R=R(h) is so small that 0h(|x|)|x|β for 0<|x|R, cf. Lemma 2.1 and the proof of part (i) .

Now we fix ε >0 so small that γεC1>0 (say, e.g., ε=γ /(2C1)), then we take δ(0,1] so small that CεC2δsp< γεC1. The latter can be done sinces > p. Thus for anyuHrad1,p(Rn)withu =δby (3.5) we have

J(u)

εC1)CεC2δsp

δp:= >0.

Clearly there isuCrad,01 (Rn), compactly supported inRn, withu =1 and|u|h >0 on some measurable subsetE of supp(u), with|E|>0. For otherwiseh=0 a.e. inRn, contradicting the definition ofWβ. Henceus,h>0. Take

τ >max

δ,[max{1, λ}/pduss,h]1/(sp)

so large thatτ u(x)U for allx∈supp(u), withd andUgiven in (3.2). By (3.2) and the fact thatp < swe obtain that

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