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On singular quasilinear elliptic equations with data measures

  • Nour Eddine Alaa EMAIL logo , Fatima Aqel and Laila Taourirte
Published/Copyright: May 16, 2021

Abstract

The aim of this work is to study a quasilinear elliptic equation with singular nonlinearity and data measure. Existence and non-existence results are obtained under necessary or sufficient conditions on the data, where the main ingredient is the isoperimetric inequality. Finally, uniqueness results for weak solutions are given.

MSC 2010: 35J60; 35J62; 35J75; 35R06

1 Introduction

In this work, we restrict our attention to the study of a class of quasilinear elliptic problem with a singular nonlinearity and data measure namely

(Pλ)Δu=a(x)uγ+b(x)|u|p+λf in Ω,u>0 in Ω,u=0 on Ω,

where Ω is an open bounded subset of ℝN for N ≥ 2, with smooth boundary Ω and f Mb+ (Ω) is a given finite nonnegative Radon measure. We assume that a and b are nonnegative functions, γ > 0, λ > 0, p ≥ 1 and ∣.∣ designates the euclidean norm in ℝN. We stress that the problem is singular as one asks to the solution to be zero on the boundary.

The study of nonlinear elliptic problems with singular nonlinearities is motivated by its various applications in many fields. For example, we can mention fluid mechanics, newtonian fluids, and glaciology [14]. They are also applicable to model problems arising from boundary layer phenomena for viscous fluids and chemical heterogeneous catalysts. Furthermore, they can be regarded as mathematical models of electrostatic MEMS devices or Micro-Electro Mechanical systems [20].

In order to trace the objectives of our work, we will start by recalling some previous studies where three types of problems were treated: quasilinear equations with regular data, semilinear problems with singular nonlinearities and coupling of both problems in the regular case.

_ Case where f is regular:

  • Case where b ≡ 0, the problem is simply written in the form

    Δu=a(x)uγ+λf(x) in Ω,u>0 in Ω,u=0 on Ω. (1.1)

    The homogeneous case (i.e. λ = 0) was considered in the pioneer works of [15, 23] and references therein. The authors showed using the method of sub- and supersolutions, that if a(x) is a bounded smooth function, then (1.1) has a classical solution.

    The case where a(x) is only a function in L1(Ω) was treated in [13] where the authors obtained some existence and regularity results for Problem (1.1) depending on the value of γ. In fact, they showed that if γ ≤ 1, Problem (1.1) has a weak solution u H01 (Ω). Otherwise if γ > 1, there exists a solution u Hloc1 (Ω) such that uγ+12H01(Ω).

    The nonhomogeneous case (i.e. λ > 0) has also been treated in [17], where the authors proved the existence of bounded solutions to (1.1) in the case where a and f belong to Lq(Ω) for q > N2.

  • Case where a ≡ 0, the problem writes

    Δu=b(x)|u|p+λf(x) in Ω,u>0 in Ω,u=0on Ω. (1.2)

    This problem was considered in [8] in the case where 1 < p ≤ 2, bL(Ω) and f is regular enough. The authors showed that if (1.2) has a subsolution u and a supersolution u in W2,q (q > N) with uu in Ω, then there exists a solution u to (1.2) such that uuu.

    This problem was also studied in [24], where the authors showed that if fW1,∞(Ω) and (1.2) has a nonnegative supersolution in W2,q(Ω) for (q > N), then it has a solution no matter the value of p (1 ≤ p < ∞). An important step in resolving such problems is to obtain an estimate on the norm of the gradient of the solution in L(Ω). The method used to get this estimate was originally introduced by Bernstein and later developed and systematized in [21, 22, 30, 31]..

_ Case where f is only integrable or a Radon measure:

  • Case where b ≡ 0 was treated in [26], where two different cases γ ≤ 1 and γ > 1 were distinguished. For γ ≤ 1, using an approximation argument, the authors obtained the existence of a weak solution u W01,q (Ω) of (1.1) for 1 ≤ q < NN1 . For γ > 1, existence and uniqueness of the solution were obtained only in Wloc1,q (Ω) for every 1 ≤ q < NN1 such that Tk(u)γ+12H01(Ω) (where Tk(u) represents the truncated function of u). The use of the truncations of u was necessary since the presence of the measure f does not allow to conclude that uγ+12 itself belongs to H01 (Ω).

  • Case where a ≡ 0 was studied in [6]. Since f is a nonnegative integrable function or, more generally a given finite nonnegative measure on Ω, it is not regular enough. Hence the usual techniques that lead to the W1,∞-solutions can not be applied. This difficulty was the main motivation behind the work [6], where the authors distinguished three cases such that, for different p values in (1.2), existence and nonexistence results are established. Firstly, considering a linear growth on the gradient, they proved the existence of a solution for (1.2) using the isoperimetric inequality. Secondly, they showed that if p > 1, the existence of a solution is obtained if λ is sufficiently small and the measure f does not charge the sets of W1,p − capacity zero 1p+1p=1. Finally, if p = 2, assuming the existence of a supersolution in W01,2 (Ω), the authors obtained the existence of a solution for Problem (1.2).

    In [19], the authors studied the existence of weak solutions for the following generalized elliptic Riccati equation

    Δu=|u|p+μ in Ω,u=0 on Ω, (1.3)

    on a bounded domain Ω ∈ ℝN for N ≥ 3 with smooth boundary Ω, where p ≥ 1 and μ is a nonnegative function or a finite positive Borel measure μM+(Ω). By involving geometric capacity estimates or pointwise behavior of Riesz potentials, together with sharp estimates of solutions and their gradients; the authors established some necessary and sufficient conditions for the existence of global solutions to (1.3).

_ Case where λ ≡ 0, b(x) ≡ 1 and 1 < p ≤ 2 was treated in [1], in which the model problem was given by

Δu=auγ+|u|p in Ω,u>0 in Ω,u=0 on Ω. (1.4)

The authors proved that if p = 2, (1.4) admits a distributional solution for all aL1(Ω). The case where 1 < p < 2 was treated differently depending on the function a. Indeed, if a(x) ∈ L(Ω), then the existence was obtained for every γ > 0. However, for the general case a(x) ∈ L1(Ω), the existence of a solution to (1.4) was proved under the condition γ > γ0, where the exact value of the constant γ0 was given.

We conclude this section by recalling some works on the parabolic version of our problem. Recently, the authors in [12] considered the following singular nonlinear parabolic equation

utΔu=auγ+μur in Ω×(0,T),u=0 on Ω×(0,T),u(0)=f in Ω,u>0 in Ω×(0,T), (1.5)

where γ > 0, μ ≥ 0, r > 0 and f Mb+ (Ω).

If r > 1, the existence of a solution to (1.5) was established for suitable small data a and f. Otherwise, if 0 < r < 1, there exists a solution for every data.

Closely related to Problem (1.5) is the following one given by (1.6), which has been considered for the p-laplacian operator in [27]

utΔpu=auγ+f in Ω×(0,T),u=0 on Ω×(0,T),u(0)=u0 in Ω, (1.6)

where p>21N+1 and γ > 0.

The authors in [27] proved that if aL1(Ω × (0, T)), u0L1(Ω) and f Mb+ (Ω × (0, T)), then there exists a nonnegative distributional solution uL1(0, T; Wloc1,1 (Ω)).

Other results concerning the well-posedness of the following triply nonlinear degenerate elliptic parabolic equation were obtained in [10],

b(u)tdiv(A(u,ϕ(u))+ψ(u)=f,ut=0=u0. (1.7)

Existence, uniqueness and continuous dependence on data u0 and f when [b + ψ](ℝ) = ℝ and ϕ ∘ [b + ψ]−1 is continuous, were established.

The main new aspect of this paper is the fact that λ and the functions a and b are not identically zero.

Our aim in this work is to prove the existence of a suitable weak solution to (Pλ). Here, as well as in the proof of other similar results, the first step is to precise in which sense we want to solve our problem. On one hand, a solution to (Pλ) has to be understood in the weak distributional meaning. On the other hand, we have to take into account the singular nonlinearity at zero. For this purpose, we adopt the following definitions:

Definition 1.1

Let u Wloc1,1 (Ω). We say that u ≤ 0 on Ω if (uϵ)+ W01,1 (Ω) for every ϵ > 0. Furthermore, u = 0 on Ω if u is nonnegative in Ω and u ≤ 0 on Ω.

Definition 1.2

If γ > 0, then a weak solution to Problem (Pλ) is a function

uWloc1,1(Ω)andu=0in Ω in the sense of Definition 1.1,ωΩ,cω,ucω>0inω,Ωuφ=Ωa(x)uγφ+Ωb(x)|u|pφ+λΩfφ,φCc1(Ω). (1.8)

The rest of our paper is organized as follows. Section 2 is devoted to necessary conditions on the data to get existence of weak solutions in (Pλ). In section 3, we investigate the existence of a solution for Problem (Pλ), when p = 1. Three different cases will be treated separately depending on the value of γ : the non-singular sublinear problem for any γ > 0, the singular sublinear problem for γ < 1 and the strongly singular problem for γ ≥ 1. Finally, in section 4, we show the uniqueness of a solution of (Pλ) when it exists, for every 1 ≤ p < NN+1 and γ > 0.

Now, in what follows, we give necessary conditions for existence. For this purpose, we prove that for sufficiently large value of λ, the equation (Pλ) has no weak solution.

2 Necessary conditions for existence

2.1 Size condition

Theorem 2.1

Let p > 1, γ > 0 and λ > 0. We suppose that aL1(Ω)+ and there exists a ball B0 in Ω such that, b(x) ≥ C0 > 0 a.e xB0 and B0f>0. Then there exists 0 < λ* < ∞ such that (Pλ) does not have any solution for λ > λ*.

Furthermore, when (Pλ) has a solution, then

φC0(B0)λB0φfCpB0|φ|pφp1, (2.1)

where Cp=p1ppp1C01p1.

Proof

See Theorem 2.1 [Alaa-Pierre, [Theorem 2.1, [6]]] for a similar detailed proof.□

Remark 2.2

The condition (2.1) is at the same time a size and regularity condition on f. It is similar to the results obtained for quasilinear elliptic equations and multidimensional Riccati equations. In other words,

  1. a regularity condition is required on f as soon as p > 1;

  2. moreover, a size condition is also required if p > 2.

For various discussions on the meaning of (2.1) and its relationship with nonlinear capacities, we refer the reader to [6] and [19].

Proposition 2.3

[Alaa-Pierre, [Proposition 2.2, [6]]] Under the hypothesis of Theorem 2.1, if Problem (Pλ) has a solution for some λ > 0, then the measure f does not charge the sets of W1,p-capacity zero.

Remark 2.4

We recall that a compact set KΩ is of W1,p-capacity zero if there exists a sequence of C0- functions φn greater than 1 on K and converging to 0 in W1,p. The above statement in Proposition 2.3 implies that

Kcompact,W1,pcapacity(K)=0Kf=0.

Obviously, this is not true for any measure f as soon as N > p′ or p > NN1. See [11] for more details.

Proof

of Proposition 2.3 See [6] for a similar detailed proof.□

In the following section, we restrict our attention to the existence of a weak solution to (Pλ) for p = 1. To this aim, we proceed by an approximation argument. The main step is to get a priori estimates on the approximate solution sequences, for any value of γ > 0.

3 Existence Results for any finite nonnegative Radon measure

In this section, we present existence results of which the proofs are based on the isoperimetric inequality [25], for linear growth on the gradient (p = 1), and for any finite measure f Mb+ (Ω). Three different problems will be treated separately in each subsection: the non-singular sublinear problem for any γ > 0, the singular sublinear problem for γ < 1 and the strongly singular problem for γ ≥ 1.

3.1 Existence of solutions to the non-singular sublinear problem

Let us consider the following regularized problem in which we regularize the singular term a(x)uγ by a(x)(u+ε)γ where ε > 0, to become not singular at the origin. The problem then rewrites

(Pε)Δu=a(x)(u+ε)γ+b(x)|u|+λfinΩ,u=0onΩ. (3.1)

Theorem 3.1

Let aL1(Ω)+ and bLN+η(Ω)+. Then, for all γ > 0, λ > 0 and for all f Mb+ (Ω), Problem (Pε) has a nonnegative weak solution u in W01,q (Ω) for 1 ≤ q < NN1.

The main tool in the proof of this theorem is the isoperimetric inequality that we will use under the following form [25].

Lemma 3.2

Let u W01,1 (Ω). Then

ddt[u>t]|u|NωN1Nμ(t)11N, (3.2)

where ωN is the Lebesgue measure of the unit ball of ℝN, and

μ(t)=meas{xΩ:|u(x)|>t}. (3.3)

Proof

of Theorem 3.1

  1. Let us approximate our Problem (Pε). For this purpose, we define the truncated function Tk as follows

    Tk(r)=max(k,min(r,k)). (3.4)

    Now, we truncate the functions a, b and f by considering the three sequences an, bn and fn which are defined by

    let nN,an(x)=min(a(x),n),bn(x)=min(b(x),n), (3.5)

    and

    fnC0(Ω), such that fn0,||fn||L1(Ω)||f||Mb(Ω) and fnf in Mb(Ω). (3.6)

    Let us now consider the following approximated problem

    unW01,(Ω),1nunΔun=an(x)(un+ε)γ+bn(x)|un|1+1nbn(x)|un|+λfninΩ. (3.7)

    The constant M¯=max((2n||an||)1γ+11n+2λn||fn||) is a supersolution of (3.7) and M = 0 is a subsolution. Then by applying the classical theory (see p.34 of [7] and the Main theorem of [2]), we obtain the existence of un solution of (3.7).

  2. At this level, we will prove the existence of a constant C independent of n such that

    Ω|un|qM,1q<NN1. (3.8)

    First of all, we introduce the following function

    pt,h(r)=0ifrt,rthiftrt+h,1ifr>t+h. (3.9)

    We multiply (3.7) by pt,h(un) and then we integrate on Ω to obtain

    Ω1nunΔunpt,h(un)=Ωan(un+ε)γ+bn|un|1+1nbn|un|+λfnpt,h(un). (3.10)

    We observe that

    bn|un|1+1nbn|un|b|un|, (3.11)

    thus,

    1h[tunt+h]|un|2[tunt+h]an(un+ε)γunth+[unt+h]an(un+ε)γ+[unt]b|un|+λ||fn||L1(Ω). (3.12)

    Since 0unth1 on the set [tunt + h] and ∣∣fn∣∣L1(Ω) ≤ ∣∣f∣∣Mb(Ω), we obtain

    1h[tunt+h]|un|2[unt]an(un+ε)γ+||b||LN+η(Ω)[unt]|un|q1q+λ||f||Mb(Ω), (3.13)

    where q=N+η=NN1ε(η),ε(η)>0.

    Hence

    1h[tunt+h]|un|2[unt]an(t+ε)γ+||b||LN+η(Ω)[unt]|un|q1q+λ||f||Mb(Ω). (3.14)

    Finally, we get

    1h[tunt+h]|un|2C1εγ+Cq[unt]|un|q1q+Cλ, (3.15)

    where C1 = ∣∣a∣∣L1(Ω), Cq = ∣∣b∣∣LN+η(Ω) and Cλ = λ ∣∣f∣∣Mb(Ω). Now, we assume that N ≥ 2 so that q < 2, and we use the following two inequalities

    1h[tunt+h]|un|q1h[tunt+h]|un|2q2(μ(t)μ(t+h)h)2q2 (3.16)

    and

    1h[tunt+h]|un|1h[tunt+h]|un|q1q(μ(t)μ(t+h)h)q1q. (3.17)

    Next, we take the qth power of (3.17) and we multiply it by the square of (3.16) to find

    1h[tunt+h]|un|q1h[tunt+h]|un|q1h[tunt+h]|un|2q(μ(t)μ(t+h)h). (3.18)

    Now, we plug the inequality (3.26) into the previous inequality, and we let h tend to zero, to obtain a differential inequality satisfied by σn(t)=[unt]|un|q and defined in the following sense

    ddt[unt]|un|qσn(t)C1εγ+Cqσn(t)1q+Cλq. (3.19)

    On the other hand, according to the isoperimetric inequality (3.2), we get

    NqωnqNμn(t)q(11N)(σn(t))C1εγ+Cqσn(t)1q+Cλqμn(t). (3.20)

    Using Young’s inequality on the right hand side term leads to

    σn(t)NqωnqND1εγq+Dqσn(t)+Dλμn(t)q(1N1)(μn(t))), (3.21)

    where D1 = C1q, Dq = Cqq and Dλ = Cλq. This implies that

    σn(t)D1^εγq+Dq^σn(t)+Dλ^μn(t)q(1N1)(μn(t))), (3.22)

    where D1^=NqωnqND1,Dq^=NqωnqNDq and D^λ=NqωnqNDλ.

    This can be rewritten as

    ddtekμn(t)ασn(t)ddtekμn(t)α1Dq^D1^εγq+Dλ^, (3.23)

    where α=1qN1N and kα=Dq^.

    Then by integrating from t = 0 to t = ∣∣un∣∣, and knowing σn(∣∣un∣∣) = 0 and μn(∣∣un∣∣) = 0, we obtain

    ekμn(0)ασn(0)1Dq^D1^εγq+Dλ^. (3.24)

    Since μn(0) ≤ ∣Ω∣, we get

    Ω|un|qC, (3.25)

    where C=ek|Ω|α1Dq^D1^εγq+Dλ^.

  3. We have

    an(un+ε)γL1(Ω)||a||L1(Ω)εγ, (3.26)

    and then from (3.7) and (3.25), we deduce

    ||Δun||L1(Ω)Cand||un||W01,q(Ω)C. (3.27)

    This yields to the compactness of un in W01,q(Ω) for 1q<NN1. Then there exists a function u such that (up to not relabeled sub-sequences), the sequence un converges to u strongly in W01,q (Ω), and (un, ∇ un) converges to (u, ∇ u) a.e in Ω.

    Moreover, by compact embedding, we obtain that un converges strongly to u in L1(Ω).

    Thus, taking φ in Cc1 (Ω), we have that

    anφun+εγ||φ||L(Ω)εγa. (3.28)

    Applying Lebesgue’s dominated convergence theorem, we obtain

    limnΩanφun+εγ=Ωaφuγ. (3.29)

    Finally, since bLN+η(Ω), then b ∣∇ un∣ converges strongly to b ∣∇ u∣ in L1(Ω). This concludes the proof since it is straightforward to pass to the limit in the last term containing fn.□

3.2 Existence of solutions to the singular sublinear problem and for every nonnegative Radon measure

Theorem 3.3

Let 0 < γ < 1, aL(Ω)+ and bLN+η(Ω)+. Then for all λ > 0 and all f Mb+ (Ω), Problem (Pλ) has a solution u in W01,q (Ω) for every 1 ≤ q < NN1.

The proof of Theorem 3.3 strictly follows the main steps of the previous proof of Theorem 3.1. We will then sketch it by enlightening the main differences. Estimates will mainly be based on the isoperimetric inequality, and so they will be formally very similar to the previous proof. The main challenge in this case will be to control the singular term 1unγ, for which we will show that un is bounded from below on the compact subsets of Ω.

Proof

  1. Let us now consider the following approximated problem

    unW01,q(Ω),1q<NN1,Δun=a(x)un+1nγ+b(x)|un|+λfinΩ. (3.30)

    The existence of a solution for (3.30) is ensured by Theorem 3.1 by letting ε = 1n in Problem (Pε).

  2. Here, we show that un is bounded from below on the compact subsets of Ω. In particular, we check that the sequence un is such that for every ω ⊂ ⊂ Ω, there exists a constant cω > 0 such that

    un(x)cωinω,for everynN. (3.31)

    In fact, we have

    Δunλf. (3.32)

    Hence, using the uniform Hopf principle as formulated in [3] and [16], there exists a constant C only depending on Ω such that

    GfC(Ω)Ωfϕ1ϕ1, (3.33)

    where ϕ1 denotes the first eigenfunction of −Δ with Dirichlet homogeneous boundary conditions, and G denotes the inverse in L1(Ω) of the operator −Δ under homogeneous Dirichlet conditions. Therefore we have

    unλGfλC(Ω)Ωfϕ1ϕ1. (3.34)

    Thus, for all compact subset ω of Ω, there exists a constant cω (not depending on n) such that uncω, in which cω can be taken as cω = λ (Ω) min {ϕ1}(x), xω}, where C~(Ω)=C(Ω)Ωfϕ1.

  3. Let us take φ = pt,h(un) as a test function in the weak formulation (3.30), where pt,h is given by (3.9). Applying (3.34), we have 1unγCϕ1γ, in which C = (λ (Ω))γ. Using the fact that un + 1n un, we obtain

    Ωunpt,h(un)CΩa(x)pt,h(un)ϕ1γ+Ωb(x)|un|pt,h(un)+λΩfpt,h(un),

    which implies that

    1h[tunt+h]|un|2C[tunt+h]a(x)ϕ1γ(unt)h+C[unt+h]a(x)ϕ1γ+[unt]b(x)|un|+λ||f||Mb(Ω).

    Since 0unth1 on the set [tunt + h], we obtain

    1h[tunt+h]|un|2CΩa(x)ϕ1γ+[unt]b(x)|un|+λ||f||Mb(Ω).

    Therefore

    1h[tunt+h]|un|2CΩa(x)ϕ1γ+||b||LN+η(Ω)[unt]|un|q1q+λ||f||Mb(Ω),

    in which q=N+η=NN1ε(η),ε(η)>0.

    Thus

    1h[tunt+h]|un|2C1Ω1ϕ1γ+Cq[unt]|un|q1q+Cλ,

    where C1 = C ∣∣a∣∣L(Ω), Cq = ∣∣b∣∣LN+η(Ω) and Cλ = λ ∣∣f∣∣Mb(Ω).

    Analogously to the proof of the previous theorem, we finally get

    Ω|un|qC. (3.35)
  4. Similarly to the passage to the limit in (3.7), we may assume that un converges strongly to u in L1(Ω) and a.e. in Ω.

    Thus, taking φ in Cc1 (Ω), we have that

    anφ(un+1n)γ||φ||L(Ω)ϕ1γa. (3.36)

    Finally, applying Lebesgue’s dominated convergence theorem, we obtain

    limnΩanφ(un+1n)γ=Ωaφuγ. (3.37)

    By a straightforward re-adaptation of the previous theorem, u is a solution to (Pλ).□

3.3 The strongly singular case: γ ≥ 1

In this case, only local estimates on the approximated solution un can be obtained. Our aim here is mainly to give global estimates on Tkγ+12(u) in H01 (Ω) in order to provide at least a weak sense to u on the boundary of Ω.

Theorem 3.4

Let γ ≥ 1, aL1(Ω)+ and bLN+η(Ω)+. Then for all f Mb+ (Ω) and λ > 0, (Pλ) has a solution u in Wloc1,q (Ω) for every 1 ≤ q < NN1. Furthermore, Tk(u)γ+12H01(Ω).

Proof

Analogously to Step 1 and Step 2 in the proof of Theorem 3.3, we obtain the existence of a solution un for the approximated Problem (3.30) for γ ≥ 1, such that for all ω ⊂ ⊂ Ω, there exists a constant cω > 0 such that

un(x)cωinω. (3.38)

In what follows, we show that Tk(u)γ+12H01(Ω).

To this aim, let H be a function in C1(ℝ) defined by

H(s)=0if|s|1,sif|s|12. (3.39)

We introduce the test function

ϕ=Hunkγeβun. (3.40)

Next, we multiply (3.30) (with γ ≥ 1) by ϕ and we integrate on Ω to obtain

γkΩ|un|2H(unk)H(unk)γ1eβun+βΩ|un|2H(unk)γeβun=Ωan(un+1n)γH(unk)γeβun+Ωbn|un|H(unk)γeβun+ΩλfH(unk)γeβun. (3.41)

Hence

c(k)ΩH(unk)γ+122+βΩ|un|2H(unk)γeβun[unk]an(un+1n)γH(unk)γeβun+[un>k]an(un+1n)γH(unk)γeβun+Ωbn|un|H(unk)γeβun+ΩλfH(unk)γeβun. (3.42)

By using the definition of H given by (3.39), the second term of the right-hand side of the inequality (3.42) vanishes and for the first term, we have

[unk]an(un+1n)γH(unk)γeβuneβkΩan(un+1n)γ(unk)γ. (3.43)

Since unγ(un+1n)γ1, then

[unk]an(un+1n)γH(unk)γeβunCk||a||L1(Ω). (3.44)

Using Young’s inequality in the third term of (3.42), we obtain

c(k)ΩH(unk)γ+122+βΩ|un|2H(unk)γeβunCk||a||L1+εΩ|un|2H(unk)γeβun+C(ε,k)Ωb2+ΩλfH(unk)γeβun. (3.45)

Concerning the last term in (3.45), we have

λΩfH(unk)γeβun=λ[unk]fH(unk)γeβun+λ[un>k]fH(unk)γeβun. (3.46)

Since H(unk)γeβun(unk)γeβuneβk on the set [unk], we get

λΩfH(unk)γeβunCk||f||Mb. (3.47)

Thus

c(k)ΩH(unk)γ+122+βεΩ|un|2H(unk)γeβunCk||a||L1+C(ε,k)Ωb2+Ck||f||Mb. (3.48)

Choosing β such that βε > 0 leads to

c(k)ΩH(unk)γ+122Ck||a||L1+C(ε,k)Ωb2+Ck||f||Mb. (3.49)

Finally, we get

ΩH(unk)γ+122C^(k). (3.50)

Now, we observe that

[unk2]H(unk)γ+122ΩH(unk)γ+122C^(k). (3.51)

From the definition of H, we obtain that

1kγ+1[unk2]|unγ+12|2C^(k). (3.52)

Consequently

Ω|Tk2(un)γ+12|2C(k). (3.53)

Even if we replace k2 by k, we obtain the desired result.

Next, we show the boundedness of un in Wloc1,q (Ω) into two steps.

For fixed k > 0, we will make use of the two truncations functions Tk(r) given by (3.4) and Gk(r) defined as

Gk(r)=|r|k+sign(r).

  1. G1(un) is bounded in W01,q (Ω) for all 1 ≤ q < NN1.

    In other words, we have to prove that there exists a constant Ck¯ depending only on k such that

    [un1]|un|qCk¯. (3.54)

    Analogously to the case γ < 1, we take ϕ = pt,h(un) as a test function in (3.30), and we obtain

    ΩΔunpt,h(un)=Ωan(un+1n)γ+bn|un|+λfnpt,h(un). (3.55)

    Hence

    1h[tunt+h]|un|2[unt]an(un+1n)γ+[unt]b|un|+λ||f||Mb(Ω).

    Therefore

    1h[tunt+h]|un|2Ωan(t+1n)γ+||b||LN+η(Ω)[unt]|un|q1q+λ||f||Mb(Ω), (3.56)

    where q=N+η=NN1ε(η),ε(η)>0. Then, we get

    1h[tunt+h]|un|2||a||L1(Ω)tγ+||b||LN+η(Ω)[unt]|un|q1q+λ||f||Mb(Ω). (3.57)

    We thus get the following inequality

    1h[tunt+h]|un|2C1tγ+Cq[unt]|un|q1q+Cλ, (3.58)

    where C1 = ∣∣a∣∣L1(Ω), Cq = ∣∣b∣∣LN+η(Ω) and Cλ = λ ∣∣f∣∣Mb(Ω).

    Let us now plug the inequality (3.58) into the previous inequality (3.18). By tending h to zero, we obtain a differential inequality satisfied by the function σn which is defined in the following sense σn(t)=[unt]|un|q,

    (ddt[unt]|un|)q(σn(t))C1tγ+Cqσn(t)1q+Cλq(μn(t)). (3.59)

    On the other hand, according to the isoperimetric inequality (3.2), we get

    NqωnqNμn(t)q(11N)(σn(t))C1tγ+Cqσn(t)1q+Cλqμn(t). (3.60)

    Using Young’s inequality on the right-hand side term leads to

    σn(t)NqωnqND1tγq+Dqσn(t)+Dλμn(t)q(1N1)(μn(t))), (3.61)

    where D1 = C1q, Dq = Cqq and Dλ = Cλq. This implies that

    σn(t)D1^tγq+Dq^σn(t)+Dλ^μn(t)q(1N1)(μn(t))), (3.62)

    where D1^=NqωnqND1,Dq^=NqωnqNDq and D^λ=NqωnqNDλ.

    This can be rewritten as

    ddtekμn(t)ασn(t)ddtekμn(t)α1Dq^D1^tγq+Dλ^, (3.63)

    where α=1qN1N and kα=Dq^.

    Integrating between 1 and ∣∣un∣∣, since σn(∣∣un∣∣) = 0 and μn(∣∣un∣∣) = 0, we get

    [un1]|un|qC^N[ekμn(1)α1]. (3.64)

    This concludes the statement of Step 1.

  2. T1(un) is bounded in Hloc1 (Ω).

    We have to investigate the behavior of (un) for its small values (un ≤ 1). To do so, we need to prove that ∀ ω ⊂ ⊂ Ω,

    ω|T1(un)|2C. (3.65)

    First, we take T1γ (un) as a test function in (3.30), and we get

    γω|T1(un)|2T1γ1(un)=Ωan(un+1n)γ+bn|un|+λfnT1γ(un)C. (3.66)

    Furthermore, according to (3.38), we have uncω on ω, and we observe that

    γcωγ1ω|T1(un)|2γΩ|T1(un)|2T1γ1(un)C. (3.67)

    Now since un = T1(un)+ G1(un), we deduce that un is bounded in Wloc1,q (Ω) for every 1 ≤ q < NN1.

    By (3.30), we obtain

    ||Δun||Lloc1(Ω)C(ω),

    This yields to the compactness of (un) in Wloc1,q (Ω) for 1 ≤ q < NN1 by applying the following Lemma:

Lemma 3.5

[Baras-Pierre, [Lemma A.2, [11]]]

Let unWloc1,q(Ω),1q<NN1 such that

||un||Wloc1,qCand||Δun||Lloc1(Ω)C. (3.68)

Then we can extract a subsequence of (un) still denoted un such that

unuinWloc1,q(Ω),unualmost everywhere inΩ.

Proof

See Lemma A.2 of [11] for a detailed proof.□

Now, for the passage to the limit in (3.30), let ω ⊂ ⊂ Ω and φ C0 (Ω), such that supp φ = ω.

Since uncω in ω, we have

an(un+1n)γφ||φ||L(Ω)cωγaL1(Ω). (3.69)

Hence, applying Lebesgue’s dominated convergence theorem, we deduce that an(un+1n)γ converges to auγ in Lloc1 (Ω).

Finally, we deduce that u is a solution to (Pλ) by a straightforward re-adaptation of the passage to the limit in the previous theorem.□

4 Uniqueness of weak solutions

Theorem 4.1

Let aL1(Ω)+, bLN+η(Ω)+ and 1 ≤ p < NN1. Then for all γ > 0, λ > 0 and f Mb+ (Ω), the solution of (Pλ) is unique if it exists.

In order to prove this result, we start by recalling the following technical lemma

Lemma 4.2

Let us consider j(r) = ∣rp. The function j is convex and we have

rRn,Aj(r)such thatr^Rn,j(r)j(r^)<A,rr^>, (4.1)

where ∂j(r) is the sub-differential of j(r) defined as follows:

  1. if p > 1, ∂j(r) := ∇ j(r) = prp−2 r,

  2. if p = 1,

    j(r)=r|r|r0,{rRn;|r|1}r=0. (4.2)

    Consequently, we deduce that for uW1,p(Ω), there exists A(x) ∈ ∂j(∇ u) such that

    u^W1,p(Ω),|u|p|u^|p<A,(uu^)>. (4.3)

    Furthermore, for 1<p<NN1, we deduce from statement (i) in Lemma 4.2 that A ∈ (Lp(Ω) )N, in which the conjugate p′ verifies 1p+1p=1 and p′ > N. Hence A ∈ (LN+η(Ω) )N for η > 0.

    For p = 1, we may deduce from (4.2), that ∣∣A(x)∣∣ ≤ 1, for all xΩ. Hence A ∈ (L(Ω) )N. Thus, again we have A ∈ (LN+η(Ω) )N.

    Finally, the uniqueness result that we obtain is a consequence of the following two lemmas:

Lemma 4.3

[Alaa-Pierre,[Lemma 4.6, [6]]]

Let a⃗LN+ε(Ω,ℝn), ε > 0, α ≥ 0 and ω a solution of

ωW01,1(Ω),αωΔωa.ωinD(Ω). (4.4)

Then ω ≤ 0.

Lemma 4.4

Let A ∈ (LN+η(Ω) )N and θ Wloc1,q (Ω) for 1 ≤ q < NN1, such that θ ≥ 0 in Ω and θ = 0 on Ω in the sense of Definition 1.1. Furthermore, we assume that θ verifies

ΔθA.θinD(Ω). (4.5)

Then θ = 0 in Ω.

Proof

of Lemma 4.4

We have (θε)+ W01,q (Ω) for all ε > 0, and by mean of Kato’s inequality up to the boundary (see [28]), we obtain

Δ(θε)+Δ(θε)χ[θε>0]Δθχ[θε>0]A.θχ[θε>0]

Hence

(θε)+W01,1(Ω),Δ(θε)+A.(θε)+inD(Ω). (4.6)

Now using the previous Lemma 4.3, we obtain

θε0,i.e.θε,ε>0, (4.7)

and since θ ≥ 0 in Ω, then θ = 0 in Ω.□

Proof

of Theorem 4.1 Let u be a supersolution of (Pλ) and û a subsolution, and let w = uû.

We take the difference between the equations associated to u and û respectively, we obtain

Δw=a(x)uγa(x)u^γ+b(x)|u|p|u^|p. (4.8)

By the convexity, there exists ALN+η(Ω, ℝn) for η > 0 such that

|u|p|u^|pA.(uu^). (4.9)

Hence

Δwa(x)uγa(x)u^γ+A~.(uu^), (4.10)

Then by Kato’s inequality, we obtain

Δw+χ[uu^>0][a(x)uγa(x)u^γ+A~.(uu^)]. (4.11)

which implies that

Δw+A~.w+. (4.12)

Therefore, thanks to Lemma 4.4, we get w = 0, which completes the proof.□

Acknowledgments

The authors wish to thank you, our esteemed referees, for your effort and time spent evaluating our article. The authors would also like to thank Professor Michel Pierre of the ENS Rennes for his remarks and corrections which improved the writing of this work in several points.

  1. Conflict of interest: Authors state no conflict of interest.

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Received: 2020-05-07
Accepted: 2021-03-28
Published Online: 2021-05-16

© 2021 Nour Eddine Alaa et al., published by De Gruyter

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

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