Home Existence and Regularizing Effect of Degenerate Lower Order Terms in Elliptic Equations Beyond the Hardy Constant
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Existence and Regularizing Effect of Degenerate Lower Order Terms in Elliptic Equations Beyond the Hardy Constant

  • David Arcoya ORCID logo EMAIL logo , Alexis Molino ORCID logo and Lourdes Moreno-Mérida ORCID logo
Published/Copyright: February 22, 2018

Abstract

In this paper, we study the regularizing effect of lower order terms in elliptic problems involving a Hardy potential. Concretely, our model problem is the differential equation

- Δ u + h ( x ) | u | p - 1 u = λ u | x | 2 + f ( x ) in  Ω ,

with Dirichlet boundary condition on Ω, where p>1 and fLhm(Ω) (i.e. |f|mhL1(Ω)) with mp+1p. We prove that there is a solution of the above problem even for λ greater than the Hardy constant; i.e., λ=(N-2)24 and nonnegative functions hL1(Ω) which could vanish in a subset of Ω. Moreover, we show that all the solutions are in Lhpm(Ω). These results improve and generalize the case h(x)h0 treated in [2, 10].

MSC 2010: 35J25; 35B65

1 Introduction

For a bounded domain ΩN (N>2) with smooth boundary Ω and 0Ω, we consider the problem

(1.1) { - Δ u + h ( x ) | u | p - 1 u = λ u | x | 2 + f ( x ) in  Ω , u = 0 on  Ω ,

where λ>0, p>1, 0hLloc1(Ω) and fLh(p+1)/p(Ω), i.e. |f|(p+1)/phL1(Ω).

In case h0, the existence of a solution for every fW-1,2(Ω) when λ<=(N-2)24 is proved in [8] ( is called the Hardy constant). Since this pioneering paper, the case h0 has been studied by many authors. When λ=0 (i.e. no Hardy potential appears in (1.1)), it was proved in [4, 6] that the lower order term h(x)|u|p-1u has a regularizing effect. More recently, it was proved in [2, 10] that if h(x)h0>0, then the lower order term has a regularizing effect: there exists a solution belonging to W01,2(Ω)Lpm(Ω) for every λ>0 provided that p+1pm<N2p-1p. The solution is obtained as limit of solutions of a sequence of suitable approximate problems. In particular, the Lpm(Ω)-regularity of the solution is only obtained for this specific solution obtained by approximation. We remark explicitly that the assumption that h(x) is uniformly away from zero is essential in these papers.

Our first goal is to deal with the existence of solutions for λ and terms h which can vanish in a subset of Ω. Indeed, in Section 2 we handle functions h(x) that can be zero in a neighborhood

Ω δ = { x Ω : dist ( x , Ω ) < δ }

of Ω. First we prove in Theorem 2.1 (a) that if

(1.2) Ω Ω δ | x | 2 ( p + 1 ) 1 - p h ( x ) 2 1 - p < ,

then there exists a solution u of (1.1) for every λΛ(δ), where Λ(δ) as δ0. Observe that in the particular case that h(x)a>0, the above condition is satisfied provided that p>2*-1. Hence, our result contains also the existence result of [2, 10] when m=p+1p (see Corollary 2.3). The case that h is zero in Ωδ is also considered in Corollary 2.5.

For the proof of Theorem 2.1 (a) we take advantage of the variational nature of (1.1) by finding its solution as a critical point of the associated Euler 𝒞1-functional Iλ (see (2.1) below). Indeed, following [3] (where the Hardy potential is substituted by a nonlinear term λu+g(x,u)), we define Iλ for functions in W01,2(Ω)Lhp+1(Ω). We show that Iλ is coercive and bounded from below. By using the Variational Principle of Ekeland we also prove that a suitable minimizing sequence of this functional is weakly convergent to a critical point uW01,2(Ω)Lhp+1(Ω) of Iλ, i.e., to a solution of (1.1).

In addition, in Theorem 2.1 (b) we also prove that if we strengthen the condition (1.2) by assuming that there exists s¯(2,p+1) such that

(1.3) Ω Ω δ | x | 2 s ¯ 2 - s ¯ h ( x ) 2 s ¯ ( p + 1 ) ( 2 - s ¯ ) < ,

then Iλ is weakly lower semicontinuous (see Remark 2.2 (iv) for a comparison with [8, Theorem 3.4]) and thus u is a minimum of the functional Iλ. We also use this additional variational characterization of this found solution to obtain the existence of a nonzero solution of problem (1.1) when f0 (see Corollary 2.6) and improve the corresponding existence results of [11, 12] (see Remark 2.7).

In Section 3, we study the regularity of every solution of (1.1). Specifically we prove in Theorem 3.1 that if fLhm(Ω) with mp+1p and |x|2pm/(1-p)h1-pm/(p-1)L1(Ω), then every solution u of (1.1) verifies uLhpm(Ω) improving the previously mentioned regularity result of [2, 10] for solutions which are only obtained as limit of solutions of approximate problems (see Remark 3.4 (ii)).

2 Coercivity and Existence of Solutions

For 0hLloc1(Ω) and r1 let Lhr(Ω) be the linear space of all measurable functions in Ω such that |f|rhL1(Ω). It can be equipped with the seminorm

| u | L h r ( Ω ) = ( Ω | u | p + 1 h ) 1 p + 1 for all  u L h r ( Ω ) ,

which is a norm in the particular case that h(x)>0 for a.e. xΩ.

We consider the reflexive space

E = W 0 1 , 2 ( Ω ) L h p + 1 ( Ω )

endowed with the norm

u E = u L 2 ( Ω ) + | u | L h p + 1 ( Ω ) .

Observe that to every function fLh(p+1)/p(Ω) there is an associated functional φf in the dual space E* (of E) given by

φ f , g = Ω f g h for all  g L h p + 1 ( Ω ) .

Hence, we understand that a solution of (1.1) is just a critical point of the 𝒞1-functional Iλ defined in E by setting

(2.1) I λ ( u ) = Ω | u | 2 2 + 1 p + 1 Ω | u | p + 1 h - λ 2 Ω u 2 | x | 2 - Ω f u h for all  u E ,

i.e. a function uE satisfying

Ω u v + Ω | u | p - 1 u v h - λ Ω u | x | 2 v - Ω f ( x ) v h = 0 for all  v E .

On the other hand, for every δ0, we define the set

Ω δ = { x Ω : dist ( x , Ω ) < δ } .

Observe that Ω0= and that clearly there exists δ0>0 such that for every δ[0,δ0] the boundary Ωδ of Ωδ is as much smooth as the boundary Ω of Ω and 0Ω¯δ, where Ω¯δ denotes the closure of Ωδ. We point out that in the sequel the positive constant δ will be always assumed to be smaller than δ0.

Our first goal is to study the existence of solutions for problem (1.1) with functions h that can vanish in Ωδ. Concretely, we are going to prove the following existence theorem.

Theorem 2.1.

Assume that p>1, fLh(p+1)/p(Ω) and that there exists δ0 such that Ωδ is smooth, 0Ω¯δ and h>0 a.e. in ΩΩδ.

  1. If condition ( 1.2 ) holds true, then there exists Λ ( δ ) such that ( 1.1 ) has a solution u E for every λ Λ ( δ ) . In addition, Λ ( δ ) as δ 0 .

  2. If, in addition, there exists s ¯ ( 2 , p + 1 ) such that condition ( 1.3 ) holds true, then u is a minimum of functional I λ given by ( 2.1 ).

Remark 2.2.

(i) As it has been previously observed, every function fLh(p+1)/p(Ω) can be considered as an element of the dual space E* of E. We will see in the proof that for the above existence result the hypothesis fLh(p+1)/p(Ω) can be relaxed to fE*.

(ii) Observe that condition (1.2) is equivalent to

1 | x | h 1 p + 1 L 2 ( p + 1 ) p - 1 ( Ω ) ,

while condition (1.3) means that

1 | x | h 1 p + 1 L 2 s ¯ s ¯ - 2 ( Ω ) .

Observe that if 2<s¯<p+1, then 2<2(p+1)p-1<2s¯s¯-2 and it follows that (1.3) implies (1.2).

(iii) Moreover, (1.3) is clearly satisfied in the case in which h(x) is a Hardy potential term of order p+1 on the left-hand side of equation (1.1), i.e. h(x)=1/|x|p+1. Indeed, in this context, condition (1.3) holds true due to the boundedness of the domain Ω.

(iv) In the case h0, part (b) of Theorem 2.1 has to be compared with [8, Theorem 3.4] where García Azorero and Peral proved the existence of a minimum of the functional by using an argument that does not require the weak lower semicontinuity of the functional Iλ, leaving this semicontinuity as an open problem. As for us, we prove that the hypothesis (1.3) implies that Iλ is weakly lower semicontinuous.

Proof of Theorem 2.1.

(a) By (1.2), using the Hölder inequality with exponent p+12, we obtain for every uE,

Ω u 2 | x | 2 = Ω δ u 2 | x | 2 + Ω Ω δ u 2 | x | 2 = Ω δ u 2 | x | 2 + Ω Ω δ u 2 h ( x ) 2 p + 1 h ( x ) 2 p + 1 | x | 2
1 ρ ( δ ) 2 Ω δ u 2 + C 1 ( Ω Ω δ | u | p + 1 h ) 2 p + 1 ,

where ρ(δ):=dist(0,Ωδ)>0.

Moreover, since u=0 in Ω and ΩΩδ, we can use a Poincaré inequality in Ωδ (see e.g. [9], [13, Section 4.6] or [1, Section 8]) to assert that

Ω δ u 2 C ( δ ) Ω δ | u | 2

with the positive constant C(δ) satisfying

(2.2) C ( δ ) = C 2 | Ω δ | C 1 , 2 ( Ω ) 0 as  δ 0 ,

where C1,2(Ω) denotes the capacity of Ω.

Hence, the functional Iλ given by (2.1) satisfies for every uE that

I λ ( u ) Ω | u | 2 2 + 1 p + 1 Ω | u | p + 1 h - λ C ( δ ) ρ ( δ ) 2 Ω δ | u | 2 2 - λ C 1 2 ( Ω Ω δ | u | p + 1 h ) 2 p + 1 - Ω f u h
( 1 - λ C ( δ ) ρ ( δ ) 2 ) Ω | u | 2 2 + 1 p + 1 Ω | u | p + 1 h - λ C 1 2 ( Ω | u | p + 1 h ) 2 p + 1 - f E * u E .

Thus, since 2p+1<1, we obtain that Iλ is coercive and bounded from below provided that

λ Λ ( δ ) := ρ ( δ ) 2 C ( δ ) .

As a consequence, by the Variational Principle of Ekeland [7], there is a bounded minimizing sequence {un}E such that

I λ ( u n ) inf E I λ

and Iλ(un)0 in E*, i.e., there exists a sequence of positive numbers {εn} converging to zero such that

(2.3) | Ω u n v + Ω | u n | p - 1 u n v h - λ Ω u n | x | 2 v - Ω f ( x ) v h | ε n v E for all  v E .

We are going to pass to the limit in this inequality as n tends to infinity. The boundedness of {un} in E implies that, up to a subsequence, we have the weak convergence of un in E to some uE. In particular, up to a subsequence, we can assume that

  1. u n u in W01,2(Ω),

  2. u n h 1 p + 1 u h 1 p + 1 in Lp+1(Ω),

  3. u n u in Lq(Ω) (1q<2*),

  4. u n ( x ) u ( x ) a.e. in Ω,

  5. there exists gLq(Ω) (1q<2*) such that |un(x)|g(x).

Obviously, by (A),

lim n Ω u n v = Ω u v for all  v W 0 1 , 2 ( Ω ) ,

and by (B) the sequence |un|p-1un is bounded in Lhp+1(Ω). Due to the a.e. convergence (D), it follows that |un|p-1un|u|p-1u in Lp+1(Ω;hdx). Hence, by (E), the Lebesgue dominated convergence theorem implies that

lim n Ω | u n | p - 1 u n v h = Ω | u | p - 1 u v h for all  v L p + 1 ( Ω ) .

In order to get the convergence of the term with Hardy potential, i.e., Ωun|x|2v, we point out that for each vW01,2(Ω) the operator Tv:W01,2(Ω) defined as

T v ( u ) = Ω u | x | 2 v for all  v W 0 1 , 2 ( Ω )

is linear and continuous since (by using Hölder and Hardy inequalities)

| T v ( u ) | ( Ω ( u | x | ) 2 ) 1 / 2 ( Ω ( v | x | ) 2 ) 1 / 2 u W 0 1 , 2 ( Ω ) v W 0 1 , 2 ( Ω )

for every vW01,2(Ω), where is the Hardy constant.

In particular, since Tv has finite range, it is also compact and hence Tv(un) strongly converges to Tv(u), i.e.

lim n Ω u n ( x ) | x | 2 v ( x ) = Ω u ( x ) | x | 2 v ( x ) .

In conclusion, taking limits in (2.3), we obtain that uE is a solution of problem (1.1) for λ<Λ(δ).

In addition, since ρ(δ)dist(0,Ω)>0 as δ0, equation (2.2) implies that Λ(δ) as δ0.

(b) As we have seen in the proof of part (a), for every λΛ(δ) the functional Iλ is bounded from below and coercive. Thus, in order to deduce that Iλ attains its minimum, it suffices to show that it is weakly lower semicontinuous. Assume hence that {un} is a sequence weakly convergent in E. As before, up to a subsequence, we can assume that {un} verifies the convergences (A)–(E). In addition, we note that the boundedness of unh1/(p+1) in Lp+1(Ω) and the a.e. convergence (D) of un imply the strong convergence of unh1/(p+1) in Ls(Ω) for every 1s<p+1. As a consequence, there exists GLs(Ω) such that (again up to a subsequence)

| u n ( x ) h 1 p + 1 ( x ) | G ( x ) for all  n .

We claim that

(2.4) lim n Ω u n ( x ) 2 | x | 2 = Ω u ( x ) 2 | x | 2 .

Indeed, if we consider the function gL2(Ω) given in (E) with q=2 which satisfies that |un(x)|g(x) for every n and almost every xΩ, then

u n 2 ( x ) | x | 2 H ( x ) for a.e.  x Ω ,

where the function H is defined in Ω as

H ( x ) = { g 2 ( x ) | x | 2 if  x Ω ¯ δ , G 2 ( x ) | x | 2 h ( x ) 2 p + 1 if  x Ω Ω ¯ δ .

By (D) we also have the convergence of un(x)2/|x|2 to u(x)2/|x|2 for almost every xΩ. Therefore, by the dominated convergence theorem, the claim will be proved if we show that HL1(Ω). For this purpose, observe that taking into account that 0Ω¯δ, we deduce that g2(x)/|x|2L1(Ω¯δ), i.e., HL1(Ω¯δ). To prove the integrability in ΩΩ¯δ, we use the Hölder inequality with exponent s2>1 to obtain

Ω Ω δ G 2 ( x ) | x | 2 h ( x ) 2 p + 1 ( Ω Ω δ 1 | x | 2 s s - 2 h ( x ) 2 s ( s - 2 ) ( p + 1 ) ) s - 2 s ( Ω Ω δ G ( x ) s ) 2 s .

The last two integral terms are finite due to hypothesis (1.3) and the fact that GLs(Ω). Consequently, we also have HL1(ΩΩ¯δ). Thus, the claim is proved.

On the other hand, Theorem 2.1 of [5] implies that (up to a subsequence) unu strongly in (Lq(Ω))N (1<q<2) and in particular (up to a subsequence) it converges almost everywhere in Ω. Then, applying the Fatou lemma, we have

(2.5) lim inf n ( Ω | u n | 2 2 + 1 p + 1 Ω | u n | p + 1 h ) Ω | u | 2 2 + 1 p + 1 Ω | u | p + 1 h .

Summarizing (2.4) and (2.5), we obtain

lim inf n I λ ( u n ) I λ ( u ) ,

i.e. the functional Iλ is weakly lower semicontinuous and the proof is concluded. ∎

If we take δ=0, then Ωδ=. Observing that

Ω | x | 2 ( p + 1 ) 1 - p <

provided that p>2*-1, we derive from Theorem 2.1 the following consequence for the case that h is a positive constant in all Ω.

Corollary 2.3.

Assume p>2*-1, fL(p+1)/p(Ω) and h(x)h0>0 in Ω. There exists a solution uE of problem (1.1) for every λR.

Remark 2.4.

In particular, we recover the existence result of [2, 10]: there exists a solution in

E = W 0 1 , 2 ( Ω ) L p + 1 ( Ω ) .

A simple case in which h vanishes in Ωδ is the following one.

Corollary 2.5.

Let p>2*-1, 0<δδ0, fL(p+1)/p(ΩΩδ) and hh0χΩΩδ for some h0>0. Then, there is a solution of (1.1) in E for λΛ(δ).

If <λ, then it is possible to choose wW01,2(Ω) such that

Ω | w | 2 - λ Ω w 2 | x | 2 < 0 .

Since p>1, we deduce in the case f0 that infEIλIλ(tw)<0=Iλ(0) provided that t is close to zero. This allows us to conclude this section by showing a simple consequence of the additional information that the solution u given in Theorem 2.1 is a minimum of Iλ.

Corollary 2.6.

If p>1, the function h satisfies (1.3) with h>0 a.e. in ΩΩδ and H<λΛ(δ), then the problem

(2.6) { - Δ u + h ( x ) | u | p - 1 u = λ u | x | 2 in  Ω , u = 0 on  Ω

has at least one nonzero solution.

Remark 2.7.

As usual, by considering instead of Iλ the functional Jλ given by

J λ ( u ) = Ω | u | 2 2 + 1 p + 1 Ω | u | p + 1 h - λ 2 Ω ( u + ) 2 | x | 2 , u E ,

it is possible to deduce the existence of a positive solution of problem (2.6). Therefore we improve the corresponding existence result of [12], where it is required additionally that h is a continuous and positive function in Ω¯, and of [11], where the case h(x)=1/|x|β with β<2 is studied. (Observe that in both cases considered in those papers, Λ(δ)= in the above corollary.)

3 Regularity of the Solutions

In this section, for the reader’s convenience we assume that hL1(Ω). In this case, by the Hölder inequality, it is easy to verify that Lhr(Ω)Lhs(Ω) for every rs1. Next, we give a sufficient condition on the function h to improve the regularity of the solution uW01,2(Ω)Lhp+1(Ω) given by Theorem 2.1. Specifically, under this condition, we show that if we strengthen the hypothesis fLh(p+1)/p(Ω) by assuming that fLhm(Ω) with mp+1p, then the solution u belongs to Lhpm(Ω).

Theorem 3.1.

Assume that hL1(Ω) with h(x)>0 a.e. in Ω and that there exists mp+1p such that

  1. f L h m ( Ω ) ,

  2. | x | 2 p m / ( 1 - p ) h 1 - p m / ( p - 1 ) L 1 ( Ω ) .

If u is a solution of (1.1), then uLhpm(Ω).

Remark 3.2.

If instead of assuming that hL1(Ω) we only assume that hLloc1(Ω), then the above hypothesis (i) should be replaced by fLh(p+1)/p(Ω)Lhm(Ω).

Proof.

For every k>0, we define the auxiliary function Tk: as usual by

T k ( s ) = { k if  s > k , s if  | s | k , - k if  s < - k .

Let uE be a solution of (1.1). Since mp+1p, we have γ:=pm-1-p>0 and we can choose |Tk(u)|γTk(u) as a test function in problem (1.1) to obtain, by dropping the positive term coming from the principal part, that

(3.1) Ω h | u | p | T k ( u ) | γ + 1 λ Ω | u | | T k ( u ) | γ + 1 | x | 2 + Ω f | T k ( u ) | γ + 1 h .

Next, we estimate each term of the above inequality. For this purpose, we define

F k ( u ) := | u | p - δ | T k ( u ) | 1 + γ + δ h ,

where

δ = ( 1 + γ ) ( p - 1 ) γ + 2 = p ( m - 1 ) ( m - 1 ) p m - p + 1 ( 0 , p - 1 ) .

Using that |Tk(s)||s| for all s, we deduce that

| u | p | T k ( u ) | γ + 1 h = F k ( u ) | T k ( u ) | - δ | u | - δ F k ( u )

and thus

(3.2) Ω h | u | p | T k ( u ) | γ + 1 Ω F k ( u ) .

On the other hand, using the Hölder inequality with exponent p-δ>1 and the fact that 1+δ+γ=(1+γ)(p-δ), we get

(3.3) λ Ω | u | | T k ( u ) | γ + 1 | x | 2 = λ ( Ω | x | 2 p m 1 - p h 1 - p m p - 1 ) 1 ( p - δ ) ( Ω F k ( u ) ) 1 p - δ C 1 ( Ω F k ( u ) ) 1 p - δ ,

where the last inequality is a consequence of hypothesis (ii).

In addition, using the Hölder inequality with exponent m and taking into account that

( γ + 1 ) m m - 1 = p m = γ + 1 + p ,

we obtain, by (i),

Ω f | T k ( u ) | γ + 1 h = Ω f h 1 m | T k ( u ) | γ + 1 h m - 1 m
( Ω | f | m h ) 1 m ( Ω | T k ( u ) | ( 1 + γ ) m m - 1 h ) m - 1 m
(3.4) C 2 ( Ω F k ( u ) ) m - 1 m .

In conclusion, substituting (3.2), (3.3) and (3.4) into (3.1), we deduce that

(3.5) Ω F k ( u ) C 1 ( Ω F k ( u ) ) 1 p - δ + C 2 ( Ω F k ( u ) ) m - 1 m .

Since 1p-δ and m-1m are less than 1, inequality (3.5) implies the existence of k0>0 and C3>0 (independent of k and u) such that

Ω | u | p - δ | T k ( u ) | 1 + γ + δ h = Ω F k ( u ) C 3 for all  k k 0 .

Fatou’s lemma when k tends to and the fact that γ+1+p=pm imply that

Ω | u | p m h ( x ) 𝑑 x = Ω | u | p + 1 + γ h C 3

as we desired. ∎

A particular interesting case is when the function h can be compared with a Hardy potential of different order.

Corollary 3.3.

Assume that fLhm(Ω) for mp+1p, and that there exist μ>0 and β0 such that the function hL1(Ω) satisfies

h ( x ) μ | x | β for a.e.  x Ω .

If u is a solution of (1.1), then uLpm(Ω;dx|x|β) for every

m { [ p + 1 p , ( N - β ) ( p - 1 ) ( 2 - β ) p ) if  β [ 0 , 2 ) , [ p + 1 p , ) if  β 2 .

Remark 3.4.

(i) The integrability of h implies that necessarily β<N.

(ii) Observe that if β[0,2), then the interval [p+1p,(N-β)(p-1)(2-β)p] of the possible values of m is not empty (i.e., p+1p<(N-β)(p-1)(2-β)p) if and only if h satisfies condition (1.2).

(iii) We note that in the particular case β=0, the regularity result is proved in [2] only for a solution obtained as limit of solutions of a sequence of suitable approximate problems, but not for every solution as in the previous result.


Dedicated to to Ireneo Peral for his seventieth birthday with deep admiration and friendship



Communicated by Patrizia Pucci


Funding statement: Supported by “Ministerio de Economía y Competitividad” MINECO-FEDER (Spain) grant MTM2015-68210-P and “Consejería de Economía, Innovación, Ciencia y Empleo, Junta de Andalucía” FQM-116.

References

[1] D. R. Adams, Choquet integrals in potential theory, Publ. Mat. 42 (1998), 3–66. 10.5565/PUBLMAT_42198_01Search in Google Scholar

[2] A. Adimurthi, L. Boccardo, G. R. Cirmi and L. Orsina, The regularizing effect of lower order terms in elliptic problems involving Hardy potential, Adv. Nonlinear Stud. 17 (2017), 311–317. 10.1515/ans-2017-0001Search in Google Scholar

[3] D. Arcoya, F. O. de Paiva and J. M. Mendoza, Existence of solutions for a nonhomogeneous semilinear elliptic equation, preprint (2017). 10.1016/j.na.2019.111728Search in Google Scholar

[4] L. Boccardo, T. Gallouët and J. L. Vázquez, Nonlinear elliptic equations in N without growth restrictions on the data, J. Differential Equations 105 (1993), 334–363. 10.1006/jdeq.1993.1092Search in Google Scholar

[5] L. Boccardo and F. Murat, Almost everywhere convergence of the gradients of solutions to elliptic and parabolic equations, Nonlinear Anal. 19 (1992), no. 6, 581–597. 10.1016/0362-546X(92)90023-8Search in Google Scholar

[6] G. R. Cirmi, Regularity of the solutions to nonlinear elliptic equations with a lower-order term, Nonlinear Anal. 25 (1995), no. 6, 569–580. 10.1016/0362-546X(94)00173-FSearch in Google Scholar

[7] I. Ekeland, On the variational principle, J. Math. Anal. Appl. 47 (1974), 324–353. 10.1016/0022-247X(74)90025-0Search in Google Scholar

[8] J. García Azorero and I. Peral, Hardy inequalities and some critical elliptic and parabolic problems, J. Differential Equations 144 (1998), 441–476. 10.1006/jdeq.1997.3375Search in Google Scholar

[9] V. Mazýa, Sobolev Spaces with Applications to Elliptic Partial Differential Equations, Springer, Berlin, 1985. Search in Google Scholar

[10] M. M. Porzio, On some quasilinear elliptic equations involving Hardy potential, Rend. Mat. Appl. (7) 27 (2007), no. 3–4, 277–297. Search in Google Scholar

[11] L. Wei and Y. Du, Exact singular behavior of positive solutions to nonlinear elliptic equations with a Hardy potential, J. Differential Equations 262 (2017), 3864–3886. 10.1016/j.jde.2016.12.004Search in Google Scholar

[12] L. Wei and Z. Feng, Isolated singularity for semilinear elliptic equations, Discrete Contin. Dyn. Syst. 35 (2015), 3239–3252. 10.3934/dcds.2015.35.3239Search in Google Scholar

[13] W. P. Ziemer, Weakly Differentiable Functions, Springer, Berlin, 1989. 10.1007/978-1-4612-1015-3Search in Google Scholar

Received: 2017-12-24
Accepted: 2018-02-06
Published Online: 2018-02-22
Published in Print: 2018-11-01

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