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Regularizing effect in some Mingione’s double phase problems with very singular data

  • In this paper we study the existence of solutions of the Dirichlet problem associated to the following nonlinear PDE

    div(a(x)u|u|p2)div(|u|(r1)λ+1u|u|λ2)=f

    where 1<λp, r>1 and fL1(Ω).

    Citation: Lucio Boccardo, Giuseppa Rita Cirmi. Regularizing effect in some Mingione’s double phase problems with very singular data[J]. Mathematics in Engineering, 2023, 5(3): 1-15. doi: 10.3934/mine.2023069

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  • In this paper we study the existence of solutions of the Dirichlet problem associated to the following nonlinear PDE

    div(a(x)u|u|p2)div(|u|(r1)λ+1u|u|λ2)=f

    where 1<λp, r>1 and fL1(Ω).



    The topic of this paper is inspired by one of the recent scientific interests of Rosario Mingione, the so–called "double phase" elliptic problem.

    The main example of a double phase integral functional is

    J(v)=Ω[1p|v|p+ρ(x)q|v|q],with 1<p<q,

    where Ω is an open, bounded subset of RN (N2),

    1<p<q,with qp close to 1 in dependence on N. (1.1)

    and

    ρ(x)0. (1.2)

    Since it is not assumed that the weight ρ(x) is bounded away from zero (that is, it is not assumed that ρ0R+ such that ρ(x)ρ0>0), it is not possible to say, even under the assumption p<q, that the term ρ(x)|v|q is dominant, so that the set {x:ρ(x)=0} plays an important role.

    Few years ago, R. Mingione found a name for such a problem: double phase problems. Since then, these problems and this terminology have become very popular.

    Note that, the functional J exhibits unbalanced growth: the (p,q)-growth in the Marcellini terminology (see [16]).

    Nowadays, there is a huge literature concerning double phase elliptic problems. Here we only recall the fundamental papers [2,3,12,13], and recently [14,17].

    The main example of a double phase elliptic nonlinear differential operator is the derivative of J, that is

    A(v)=div(v|v|p2)div(ρ(x)v|v|q2),

    In this paper we study the existence of distributional solutions, belonging to some standard Sobolev spaces, of Dirichlet problems with very singular data, and associated to differential operators of double phase type like

    div(a(x)v|v|p2)div(g(v)v|v|λ2),

    with g(0)=0.

    Namely, we deal with the existence of solutions of the following boundary value problem

    {div(a(x)u|u|p2)div(g(u)u|u|λ2)=f,inΩ;u=0,onΩ; (1.3)

    where Ω is an open, bounded subset of RN (N2),

    1<λp<N, (1.4)

    a(x) is a measurable function such that

    αa(x)β,withα,β>0, (1.5)
    g(t)=|t|(r1)λ+1, withr>1, (1.6)
    fL1(Ω). (1.7)

    We point out that

    ● in (1.4) the parameters λ,p play the role of p,q in (1.1)

    ● the operator presented in (1.3) also depends on a power of u;

    ● the coefficient a(x) does not need to be smooth.

    Our existence results hinge on the presence of the additional term

    div(g(u)u|u|λ2),

    which strongly helps, even if it has a growth (with respect to the gradient) λp and despite of the degeneracy due to the factor |u|(r1)λ+1.

    As a matter of fact, this term provides a strong regularizing property: roughly speaking, we prove that the solution u of (1.3), under a suitable relationship between the parameters p and λ, is more regular (and it even exists) than the solution y of

    {div(a(x)y|y|p2)=f,in Ω;y=0,onΩ, (1.8)

    studied in [4,7,8].

    The regularizing effect of some lower orders terms, in the framework of boundary value problems with L1-data, is already known since the paper [10] by H. Brezis and W. A. Strauss. We also refer to the paper [1,6,9,11], where some Dirichlet problems with lower order terms of order zero or of order one, with natural growth with respect to u are studied.

    This section deals with the case

    fL(Ω).

    In the sequel, given k>0, we denote by Gk(s) and Tk(s) the classical truncated functions defined by

    Gk(s)=(|s|k)+sgns,Tk(s)=sGk(s),sR.

    Let us introduce the following sequence of boundary value problems

    {div(a(x)un|un|p2)div(g(Tn(un))un|un|λ21+1n|un|λ1)=f(x),inΩ;un=0,onΩ.

    As a consequence of the classical result due to J. Leray, J. L. Lions (see [15]) there exists unW1,p0(Ω) which is a weak solution of the above problem in the sense that the following integral identity holds

    Ωa(x)un|un|p2v+Ωg(Tn(un))un|un|λ21+1n|un|λ1v (2.1)
    =Ωfv,for anyvW1,p0(Ω).

    Moreover, due to the boundedness of f and adapting the well known method used in [18], each un is a bounded function and there exists a positive contant Cf, independent on n, such that

    unL(Ω)Cf,nN.

    Thus, for any n>Cf it holds Tn(un)=un and un is a weak solution of the following Dirichlet problem

    {unW1,p0(Ω):div(a(x)un|un|p2)div(g(un)un|un|λ21+1n|un|λ1)=f(x), (2.2)

    that is

    Ωa(x)un|un|p2v+Ωg(un)un|un|λ21+1n|un|λ1v (2.3)
    =Ωfv,for anyvW1,p0(Ω).

    Taking un as test function in (2.3) and using the assumption (1.5) we have

    αΩ|un|p+Ωg(un)|un|λ1+1n|un|λ1Ωfun.

    Dropping the second (positive) term in the left–hand side and using the boundedness of f we obtain

    unW1,p0(Ω)C1,nN. (2.4)

    Here, and in the sequel, we denote by Ci positive constants only depending on the data (but not on n).

    Thus, there exist a subsequence, not relabelled, and a function uW1,p0(Ω)L(Ω) such that

    unuweakly in W1,p0(Ω), (2.5)
    unustrongly inLp(Ω), and a.e. in Ω. (2.6)

    Moreover, using estimate (2.4) we obtain, since 1<λp,

    Ω1n|un|λ1C2n,nN.

    Thus,

    1n|un|λ10strongly inL1(Ω), and a.e. in Ω. (2.7)

    In order to have

    unustrongly in W1,p0(Ω), (2.8)

    it is enough to prove that

    Ωa(x)[un|un|p2u|u|p2](unu)0. (2.9)

    Let us take v=unu as test function in (2.3)

    Ωa(x)[un|un|p2u|u|p2](unu)
    +Ωg(un)un|un|λ2u|u|λ21+1n|un|λ1(unu)
    =Ωf(unu)Ωa(x)u|u|p2(unu)
    Ωg(un)u|u|λ21+1n|un|λ1(unu)

    Due to the positivity of the second term we get

    Ωa(x)[un|un|p2u|u|p2](unu) (2.10)
    Ωf(unu)Ωa(x)u|u|p2(unu)
    Ωg(un)u|u|λ21+1n|un|λ1(unu).

    We note that the first and the second integral in the right–hand side converge to 0. Moreover,

    g(un)u|u|λ21+1n|un|λ1g(u)u|u|λ2a.e. in Ω

    and (since |u|λ1Lp)

    |g(un)u|u|λ21+1n|un|λ1|g(Cf)|u|λ1,nN.

    Thus, by the Lebesgue Theorem we get

    g(un)u|u|λ21+1n|un|λ1g(u))u|u|λ2strongly in Lp(Ω), (2.11)

    which in turn implies

    Ωg(un)u|u|λ21+1n|un|λ1(unu)0.

    Then, (2.9) easily follows taking the limit as n+ in (2.10) and the strong convergence (2.8) is proved. Finally, we take the limit as n+ in (2.3) (using (2.9) and (2.11)) and we obtain the following existence theorem.

    Theorem 2.1. Let 1<λp<N. Assume that (1.5), (1.6) hold and let

    fL(Ω).

    Then there exists a weak solution uW1,p0(Ω)L(Ω) which solves the problem (1.3) in the following weak sense

    Ωa(x)u|u|p2v+Ωg(u)u|u|λ2v=Ωfv (2.12)

    for any vW1,p0(Ω).

    In this section we assume that

    fL1logL1(Ω) (3.1)

    and we will prove the existence of a distributional solution of problem (1.3)

    Let {fn} be a sequence of bounded functions such that

    fnfstrongly inL1(Ω),

    and

    fnL1(Ω)fL1(Ω),nN.

    Classical examples are fn=Tn[f] and fn=f1+1n|f|.

    Let us introduce the following approximate boundary value problems

    {div(a(x)un|un|p2)div(g(un)un|un|λ2)=fn(x),in Ω;un=0,onΩ. (3.2)

    By Theorem 2.1, there exists unW1,p0(Ω)L(Ω) such that, for any vW1,p0(Ω),

    Ωa(x)un|un|p2v+Ωg(un)un|un|λ2v=Ωfnv. (3.3)

    Let k>0; by taking Tk(un) as test function in the weak formulation (3.3) of problem (3.2) and dropping the positive second term, we can proceed as in [4] and the following lemma holds.

    Lemma 3.1. Let 1<λp<N. Assume that the hypotheses (1.5), (1.6), (3.1) are satisfied. Then, for any k>0 it holds

    Ω|Tk(un)|pkΩ|f|,nN. (3.4)

    Moreover, there exists C0>0 such that

    Ω|un|sC0,s<(p1)NN1, (3.5)

    and

    {a(x)un|un|p2}isboundedinLt(Ω),1<t<NN1. (3.6)

    Next, we will prove the following lemma.

    Lemma 3.2. Let 1<λp<N. Assume that the hypotheses (1.5), (1.6), (3.1) are satisfied. Then there exists a positive constant R, independent on n, such that

    Ω|un|λR,nN. (3.7)

    Proof. We set η=(r1)λ+1 (note that η>1 since r>1) and we take

    v=[11(1+|un)η1]un|un|

    as test function in (3.3). Dropping the positive term resulting by the principal part, we obtain

    (η1)Ω|un|η(1+|un|)η|un|λΩ|fn(x)|[1(1+|un|)1η]Ω|f(x)|.

    We fix k>0. By the above estimate we have

    (η1)kη(1+k)η{|un|>k}|un|λfL1(Ω). (3.8)

    Thus, putting together estimates (3.4) and (3.8), it follows (3.7).

    Further improvements on the boundedness of un and un, depending on the relationship between the parameters p,λ and r, can be derived from the following lemma

    Lemma 3.3. Let 1<λp<N. Assume that the hypotheses (1.5), (1.6), (3.1) are satisfied. Then there exist two positive constants R1,R2 independent of n such that

    Ω|un|rλR1,nN (3.9)

    and

    Ω|un|σR2,nN (3.10)

    with

    σ=rpλ1+rλ.

    Proof. By taking v=log(1+|un|)un|un| as test function in the weak formulation (3.3) of problem (3.2) (see [8]), it is easy to see that

    αΩ|un|p1+|un|+Ω|un|(r1)λ+11+|un||un|λΩ|f|log(1+|un|).

    Using in the right–hand side the inequality

    stslog(1+s)+et,s,t>0

    and the boundedness of {un} in L1(Ω) and, taking into account the positivity of each of the two integrals in the left-hand side and (3.7), the following two estimates hold

    Ω|un|(r1)λ+11+|un||un|λC3,nN (3.11)

    and

    Ω|un|p1+|un|C4,nN (3.12)

    From estimate (3.11) we also deduce

    12|un|>1|un|(r1)λ|un|λC5,nN

    which, together with inequality (3.4), implies

    Ω|un|(r1)λ|un|λC6,nN. (3.13)

    Now, we can use Sobolev inequality

    1(rS)λ(Ω|un|rλ)λλ1rλΩ||un|r|λ=
    Ω|un|(r1)λ|un|λC7,nN

    and the estimate (3.9) follows.

    Next, let us prove (3.10). We follow the outline of [8]. Note that since σ<p, by Hölder inequality with exponents pσ,ppσ and inequality (3.12), we have

    Ω|un|σ=Ω|un|σ(1+|un|)σp(1+|un|)σpC8[Ω(1+|un|)σpσ]pσp

    and the proof is concluded, since, by the choice of σ, it follows σpσ=rλ.

    Remark 3.4. Note that in Lemmas 3.1 and 3.7 we only use the assumption fL1(Ω), while Lemma 3.3 requires the additional hypothesis fL1logL1(Ω). However, if f is merely summable, the proof of Lemma 3.3 can be repeated in order to obtain the boundedness of {un} in W1,σ0(Ω), for any 1σ<rpλ1+rλ.

    Remark 3.5. We point out that

    max

    Moreover

    N\frac{pr-1}{Nr-1} > 1 \quad \iff \quad p > 1+\frac{N-1}{r}.

    Thus, Lemma 3.3 improves Lemma 3.7 if 1\leq \lambda < N\frac{pr-1}{Nr-1} and p > 1+\frac{N-1}{r} . (Note that 1+\frac{N-1}{r} \in \big]1, 2-\frac{1}{N}\big[ since r > 1 ).

    Remark 3.6. Let 2-\frac{1}{N} < p < N . Taking into account only the contribution of the principal part and applying the results of [7] we deduce that the sequence \left\{{u_{n}} \right\} is bounded in W^{1, \frac{N(p-1)}{N-1}}_0(\Omega) .

    Thus the term

    -{{{\rm{\;div}}}}\big( g({u_{n}})\nabla {u_{n}}|\nabla{u_{n}}|^{\lambda-2}\big)

    has a regularizing effect in the following two cases

    i) 2-\frac1N < p < N \hbox{ and } \frac{(p-1)N}{N-1} < \lambda \leq p,

    ii) 1 < p\leq 2-\frac1N and 1 < \lambda \leq p .

    As a consequence of previous lemmas we prove the following two existence results.

    Theorem 3.7. Let 1 < \lambda \leq p < N . Assume that hypotheses (1.5), (1.6) and (3.1) hold.

    Then there exists u \in W^{1, \lambda}_0(\Omega) , such that g(u)|\nabla u|^{\lambda-1} \in L^1(\Omega) , which solves the problem (1.3) in the following distributional sense

    \begin{equation} {\int _{\Omega}} a(x)\,\nabla u|\nabla u|^{p-2} \nabla v \, +{\int _{\Omega}} g(u) \nabla u|\nabla u|^{\lambda-2} \nabla v \, = {\int _{\Omega}} fv, \, \end{equation} (3.14)

    for any v \in C^{\infty}_0(\Omega).

    Theorem 3.8. Let 1 < \lambda \leq p < N . Assume that hypotheses (1.5), (1.6) and (3.1) hold.

    Then there exists u \in W^{1, \sigma}_0(\Omega) , such that g(u)|\nabla u|^{\lambda-1} \in L^1(\Omega) , which solves the problem (1.3) in the distributional sense (3.14).

    Remark 3.9. We explicitly remark that, in the case \lambda = p , Theorem 3.7 gives the existence of at least one solution with finite energy without any additional assumption on the summability of f . A similar regularizing effect occurs for the solution of the Dirichlet problem associated to the equation

    -{{{\rm{\;div}}}}\big( a(x)\,\nabla u|\nabla u|^{p-2}\big)+ u|u|^{s-1} = f,

    where f \in L^m(\Omega) with 1 < m < (p^*)' , when a suitable balance between m and s holds, (see [11]) or to the equation

    -{{{\rm{\;div}}}}\big( a(x)\,\nabla u|\nabla u|^{p-2}\big)+u|u|^s|\nabla u|^{p} = f

    with f \in L^1(\Omega) (see [9]).

    The following Figure 1 summarizes the different regularity results in dependence of p and \lambda .

    Figure 1.  Regularity results in dependence of p and \lambda .

    If (p, \lambda) belongs to the region A , the better regularity is the one obtained in [7], i.e., u \in W^{1, \frac{N(p-1)}{N-1}}_0(\Omega) ; otherwise the better regularity is the one proved here.

    If (p, \lambda) belongs to the region B , Theorem 3.8 gives the existence of a distributional solution u \in W^{1, \sigma}_0(\Omega) ; while in the region C the better regularity is the one stated in Theorem 3.7, i.e., u \in W^{1, \lambda}_0(\Omega) .

    At last, if (p, \lambda) belongs to the colored region the result stated in Theorem 3.7 is new.

    We begin with the proof of Theorem 3.7.

    As a consequence of Lemma 3.1 and Lemma 3.7 there exist a subsequence, not relabelled, and a function u \in W^{1, \lambda}_0(\Omega) such that

    \begin{equation} \begin{cases} {u_{n}} \rightharpoonup u \quad \text{weakly in }W^{1,\lambda}_0(\Omega), \\ {u_{n}} \rightarrow u \quad \text{strongly in} \, L^{\lambda}(\Omega) \text{ and a.e. in } \Omega, \\ T_k({u_{n}}) \rightharpoonup T_k(u) \quad \text{weakly in } {W_0^{1,p}(\Omega)}. \end{cases} \end{equation} (3.15)

    In order to take the limit as n \to +\infty in (3.2) we have to prove that

    \nabla {u_{n}} \to \nabla u \quad \text{a.e. in }\Omega.

    We follow some techniques of [5]. For any \xi \in {\mathbb{R}}^N , we set

    A(x,\xi) = a(x)\xi|\xi|^{p-2}, \quad B_n(\xi) = \frac{\xi|\xi|^{\lambda-2}}{1+\frac1n|\xi|^{\lambda-1}}.

    Let j, k > 0 ; using v = T_j[u_n-T_k(u)] as test function in (3.3) we have

    \begin{array}{l} {\int _{\Omega}} [ A(x, \nabla {u_{n}})- A(x, \nabla T_k(u)) ]\nabla T_j[{u_{n}}-T_k(u)] \\ +{\int _{\Omega}} A(x, \nabla T_k(u)) \nabla T_j[{u_{n}}-T_k(u)] \\ +{\int _{\Omega}} g({u_{n}}) [B_n(\nabla {u_{n}})-B_n(\nabla T_k(u))] \nabla T_j[{u_{n}}-T_k(u)] \\ +{\int _{\Omega}} g({u_{n}}) B_n(\nabla T_k(u)) \nabla T_j[{u_{n}}-T_k(u)] = {\int _{\Omega}} f T_j[{u_{n}}-T_k(u)]. \end{array} (3.16)

    We note that

    {\int _{\Omega}} g({u_{n}}) [B_n(\nabla {u_{n}})-B_n(\nabla T_k(u))] \nabla T_j[{u_{n}}-T_k(u)] \geq 0 .

    Moreover (since A(x, \nabla T_k(u)) \nabla T_j[u-T_k(u)] = 0 )

    \lim\limits_{n \to \infty} {\int _{\Omega}} A(x, \nabla T_k(u)) \nabla T_j[{u_{n}}-T_k(u)] = 0

    and

    \begin{array}{l} \lim\limits_{n \to \infty}{\int _{\Omega}} g({u_{n}}) B_n(\nabla T_k(u)) \nabla T_j[{u_{n}}-T_k(u)] \\ = \lim\limits_{n \to \infty}\int_{\{|{u_{n}}-T_k(u)| < j\}}g({u_{n}}) \,B_n(\nabla T_k(u)) \nabla [{u_{n}}-T_k(u)] = 0 \end{array}

    since B_n(0) = 0 . Thus, from (3.16) we deduce

    \begin{array}{l} 0 \leq {\int _{\Omega}} [ A(x, \nabla {u_{n}})- A(x, \nabla T_k(u)) ]\nabla T_j[{u_{n}}-T_k(u)] \\ \leq \epsilon_n^1(k) + \epsilon_n^2(k) + \omega_n(k), \end{array} (3.17)

    where we have denoted by \epsilon_n^1(k) and \epsilon_n^2(k) two functions which go to 0 as n \to +\infty , for any k > 0 and

    \omega_n(k) = {\int _{\Omega}} f T_j[{u_{n}}-T_k(u)].

    Now, we use the above inequality in order to prove the L^1 compactness of the sequence \{\nabla u_n\} .

    Let 0 < \theta < \dfrac{\lambda}{p}\, ( 0 < \theta < 1 ) and k > 0 . Let us define

    I_{n,\Omega} = \int_{\Omega} \{[ A(x, {\nabla u_n} ) - A(x, {\nabla u} ) ] \nabla (u_n-u) \}^\theta .

    and let us prove that the previous integral converges to zero.

    Indeed, it holds

    I_{n,\Omega} = I_{n,\,C_k} + I_{n,\,A_k}

    where

    I_{n,\,C_k} = \int_{C_k} \{[ A(x, {\nabla u_n} ) - A(x, {\nabla u} ) ] \nabla (u_n-u) \}^\theta

    and

    I_{n,\,A_k} = \int_{A_k} \{[ A(x, {\nabla u_n} ) - A(x, {\nabla u} ) ] \nabla (u_n-u) \}^\theta

    with

    C_k = \{x :|u(x)| \leq k \}, \qquad A_k = \{x :|u(x)| > k \}.

    We observe that

    I_{n,C_k } \leq \int_{\Omega} \{[ A(x, {\nabla u_n} ) - A(x, {\nabla T_k(u)} ) ] \nabla (u_n-T_k(u)) \}^\theta = J_{n,\Omega}.

    Using the Hölder inequality, with exponents \frac{\lambda}{p\theta} and \frac{\lambda}{\lambda-p\theta} , and the a priori estimate (3.10), we have

    \begin{array}{l} I_{n,\Omega} \leq J_{n,\Omega} + I_{n,\,A_k} \\ \leq J_{n, \Omega } + C_11 \, \left[ \int_{A_k} (|\nabla u_n| + |\nabla u|)^{\lambda} \right]^{\frac{p\theta}{\lambda}}\,|A_k|^{1 - \frac{p\theta}{\lambda}} \\ \leq J_{n,\Omega } + C_12 \, |A_k|^{1 -\frac{p\theta}{\lambda}} = J_{n,\Omega} + \omega^1 (k). \end{array} (3.18)

    Here and in the sequel, for any measurable set E \subset {\mathbb{R}}^N, |E| denotes its N- dimensional measure. Moreover, by \omega^i (k) we denote some quantities such that \lim_{k \to \infty } \omega^i (k) = 0 . Now, we have to study the behavior of J_{n, \Omega} ; it can be splitted as ( j \in {{\mathbb{N}}} )

    J_{n, \Omega} = {\int _{\Omega}} \{[ A(x, {\nabla u_n} ) - A(x, {\nabla T_k(u)} ) ] \nabla T_j[u_n-T_k(u)] \}^\theta
    +\int_{\{ |u_n-T_k(u)| > j \}} \{[ A(x, {\nabla u_n} ) - A(x, {\nabla T_k(u)} ) ] \nabla [u_n-T_k(u)] \}^\theta = J^1_{n, \Omega}+J^2_{n, \Omega}.

    We estimate J^1_{n, \Omega} and J^2_{n, \Omega} by means of Hölder inequality with exponents \frac1\theta , \frac{1}{1-\theta} and \frac{\lambda}{p\theta} , \frac{\lambda}{\lambda-p\theta} , respectively and we use inequalities (3.17) and (3.7), getting

    J_{n, \Omega} = \bigg[ \int_{\Omega} [ A(x, {\nabla u_n} ) - A(x, {\nabla T_k(u)} ) ] \nabla T_j [u_n-T_k(u)] \bigg]^\theta \ |\Omega|^{1-\theta} \
    +C_R\, |\{ x : |u_n-T_k(u)| > j \}|^{1 - \frac{p\theta}{\lambda}}.
    \leq C_13 \, [ \epsilon^1_n(k)+\epsilon^2_n(k)+\omega_n(k) ]^\theta + C_R \, |\{ x : |u_n-T_k(u)| > j \}|^{1 - \frac{p\theta}{\lambda}}.

    Since

    \omega_n(k) \to {\int _{\Omega}} f T_j[u-T_k(u)] = \omega^2(k)

    and

    \limsup\limits_{n \to \infty} |\{ |u_n-T_k(u)| > j \}|^{1 - \frac{p\theta}{\lambda}} \leq \ |\{ |u-T_k(u)| \geq j \}|^{1 - \frac{p\theta}{\lambda}} = \omega^3 (k),

    we obtain

    \limsup\limits_{n \to \infty}J_{n, \Omega} \leq C_14 \, [ \omega^2 (k)]^\theta +C_15 \, \omega^3 (k).

    Summing up the above inequality and (3.18) we have

    \limsup\limits_{n \to \infty} [I_{n, C_k} +I_{n, A_k}]\leq \omega^1 (k) + C_16\, [\omega^2 (k)]^\theta+C_17\, \omega^3 (k).

    Therefore,

    \int_{\Omega} \{[ A(x, {\nabla u_n} ) - A(x, {\nabla u} ) ] \nabla (u_n-u) \}^\theta \to 0,

    which gives (for a suitable subsequence, still denoted by u_n )

    \{[ A(x, {\nabla u_n} ) -A(x, {\nabla u} ) ] \nabla (u_n-u) \}^\theta \to 0 \quad \text{a.e.},

    and also (since \theta is positive)

    \{[ A(x, {\nabla u_n} ) -A(x, {\nabla u} ) ] \nabla (u_n-u) \} \to 0 \quad \text{a.e.}.

    In [15], it is proved that, under our assumptions on the function A(x, {\xi}) , the previous limit implies that

    \begin{equation} \nabla u_n(x) \to \nabla u(x) \qquad \text{a.e.}. \end{equation} (3.19)

    Thus

    \begin{equation} a(x)\nabla {u_{n}}(x)|\nabla {u_{n}}(x)|^{p-2}\to a(x)\nabla u(x)|\nabla u(x)|^{p-2} , \; \text{ a.e. } \end{equation} (3.20)

    and, thanks to (3.6) we have

    \begin{equation} a(x)\nabla {u_{n}}(x)|\nabla {u_{n}}(x)|^{p-2}\to a(x)\nabla u(x)|\nabla u(x)|^{p-2} , \; \text{ in }\; L^\tau(\Omega) ,\;1 < \tau < t < \frac{N}{N-1}. \end{equation} (3.21)

    Next, we will prove that

    \begin{equation} g({u_{n}}) \nabla {u_{n}} |\nabla{u_{n}}|^{\lambda-2} \rightarrow g(u) \nabla u |\nabla u|^{\lambda-2} \quad \text{ in } L^{1}(\Omega). \end{equation} (3.22)

    Thanks to (3.19) we also deduce

    g({u_{n}}) \nabla {u_{n}} |\nabla{u_{n}}|^{\lambda-2} \rightarrow g(u) \nabla u |\nabla u|^{\lambda-2} \quad \text{a.e. in } \Omega.

    Moreover, for any measurable set E \subset \Omega we have

    \begin{array}{l} \int_E g({u_{n}}) |\nabla{u_{n}}|^{\lambda-1} = \int_E |{u_{n}}|^{r }\; \big(|{u_{n}}|^{r -1}|\nabla{u_{n}}| \big)^{\lambda-1} \\ \leq C_20 \bigg[\int_E |{u_{n}}|^{\lambda r}\bigg]^\frac1{\lambda} \bigg[\int_E |{u_{n}}|^{(r-1)\lambda }|\nabla {u_{n}}|^{\lambda}\bigg]^{1-\frac1{\lambda}} \\ \leq C_21 \bigg[{\int _{\Omega}} |{u_{n}}|^{\lambda^*r}\bigg]^\frac1{\lambda^*} |E|^{\frac{1}{\lambda}-\frac{1}{\lambda^*}} \bigg[{\int _{\Omega}}|{u_{n}}|^{(r-1)\lambda }|\nabla {u_{n}}|^{\lambda}\bigg]^{1-\frac1{\lambda}} \end{array} (3.23)

    and the right–hand side goes to 0 as |E| \to 0 uniformly w.r.t. n , since estimates (3.9) and (3.13) hold. Thus

    \lim\limits_{|E| \to 0} \int_E g({u_{n}}) |\nabla{u_{n}}|^{\lambda-1} = 0,\;\hbox{ uniformly w.r.t. }\,n.

    Thanks to Vitali Theorem the convergence (3.22) is proved and

    {\int _{\Omega}} g({u_{n}}) \nabla {u_{n}} |\nabla{u_{n}}|^{\lambda-2} \nabla v \rightarrow {\int _{\Omega}} g(u) \nabla u |\nabla u|^{\lambda-2} \nabla v, \quad \forall\; v \in C^{\infty}_0(\Omega).

    The above limit and the limit (3.21), allow us to take the limit as n \to +\infty in (3.3) and the proof of Theorem 3.7 follows.

    In order to prove Theorem 3.8 we note that as a consequence of Lemma 3.1 and Lemma 3.3. there exist a subsequence, not relabelled, and a function u \in W^{1, \sigma}_0(\Omega) such that

    \begin{equation} \begin{cases} {u_{n}} \rightharpoonup u \quad \text{weakly in } W^{1, \sigma}_0(\Omega) \\ {u_{n}} \rightarrow u \quad \text{strongly in} \, L^{\sigma }(\Omega) \text{ and a.e. in } \Omega, \\ T_k({u_{n}}) \rightharpoonup T_k(u) \quad \text{weakly in } {W_0^{1,p}(\Omega)}. \end{cases} \end{equation} (3.24)

    and the proof can be performed as above. Precisely, in order to obtain the a.e. convergence of \{\nabla {u_{n}}\} we just have to replace \lambda with \sigma .

    This work has been supported by Project EEEP & DLaD – Piano della Ricerca di Ateneo 2020-2022–PIACERI.

    G. R. Cirmi is member of the Gruppo Nazionale per l'Analisi Matematica, la Probabilità e le loro Applicazioni (GNAMPA) of the Istituto Nazionale di Alta Matematica (INdAM).

    The authors declare no conflict of interest.



    [1] D. Arcoya, L. Boccardo, Regularizing effect of the interplay between coefficients in some elliptic equations, J. Funct. Anal., 268 (2015), 1153–1166. https://doi.org/10.1016/j.jfa.2014.11.011 doi: 10.1016/j.jfa.2014.11.011
    [2] P. Baroni, M. Colombo, G. Mingione, Harnack inequalities for double phase functionals, Nonlinear Anal., 121 (2015), 206–222. https://doi.org/10.1016/j.na.2014.11.001 doi: 10.1016/j.na.2014.11.001
    [3] P. Baroni, M. Colombo, G. Mingione, Regularity for general functionals with double phase, Calc. Var., 57 (2018), 62. https://doi.org/10.1007/s00526-018-1332-z doi: 10.1007/s00526-018-1332-z
    [4] P. Bénilan, L. Boccardo, T. Gallouët, R. Gariepy, M. Pierre, J. L. Vazquez, An L^1 theory of existence and uniqueness of solutions of nonlinear elliptic equations, Ann. Scuola Norm. Sci., 22 (1995), 241–273.
    [5] L. Boccardo, Some nonlinear Dirichlet problems in L^1 involving lower order terms in divergence form, In: Progress in elliptic and parabolic partial differential equations, Harlow: Longman, 1996, 43–57.
    [6] L. Boccardo, G. R. Cirmi, Some elliptic equations with W_0^{1, 1} solutions, Nonlinear Anal., 153 (2017), 130–141. https://doi.org/10.1016/j.na.2016.09.007 doi: 10.1016/j.na.2016.09.007
    [7] L. Boccardo, T. Gallouët, Nonlinear elliptic and parabolic equations involving measure data, J. Funct. Anal., 87 (1989), 149–169. https://doi.org/10.1016/0022-1236(89)90005-0 doi: 10.1016/0022-1236(89)90005-0
    [8] L. Boccardo, T. Gallouët, Nonlinear elliptic equations with right hand side measures, Commun. Part. Diff. Eq., 17 (1992), 189–258. https://doi.org/10.1080/03605309208820857 doi: 10.1080/03605309208820857
    [9] L. Boccardo, T. Gallouët, Strongly nonlinear elliptic equations having natural growth terms and L^1- data, Nonlinear Anal., 19 (1992), 573–579. https://doi.org/10.1016/0362-546X(92)90022-7 doi: 10.1016/0362-546X(92)90022-7
    [10] H. Brézis, W. A. Strauss, Semi-linear second-order elliptic equations in L^1, J. Math. Soc. Japan, 25 (1973), 565–590. https://doi.org/10.2969/jmsj/02540565 doi: 10.2969/jmsj/02540565
    [11] G. R. Cirmi, Regularity of the solutions to nonlinear elliptic equations with a lower-order term, Nonlinear Anal., 25 (1995), 569–580. https://doi.org/10.1016/0362-546X(94)00173-F doi: 10.1016/0362-546X(94)00173-F
    [12] M. Colombo, G. Mingione, Bounded minimisers of double phase variational integrals, Arch. Rational Mech. Anal., 218 (2015), 219–273. https://doi.org/10.1007/s00205-015-0859-9 doi: 10.1007/s00205-015-0859-9
    [13] M. Colombo, G. Mingione, Regularity for double phase variational problems, Arch. Rational Mech. Anal., 215 (2015), 443–496. https://doi.org/10.1007/s00205-014-0785-2 doi: 10.1007/s00205-014-0785-2
    [14] C. De Filippis, G. Mingione, Nonuniformly elliptic Schauder theory, arXiv: 2201.07369.
    [15] J. Leray, J. L. Lions, Quelques résultats de Višik sur les problèmes elliptiques semi-linéaires par les méthodes de Minty et Browder, Bull. Soc. Math. France, 93 (1965), 97–107. https://doi.org/10.24033/bsmf.1617 doi: 10.24033/bsmf.1617
    [16] P. Marcellini, Regularity and existence of solutions of elliptic equations with p, q-growth conditions, J. Differ. Equations, 90 (1991), 1–30. https://doi.org/10.1016/0022-0396(91)90158-6 doi: 10.1016/0022-0396(91)90158-6
    [17] P. Marcellini, Local Lipschitz continuity for p, q-PDEs with explicit u-dependence, Nonlinear Anal., 226 (2023), 113066. https://doi.org/10.1016/j.na.2022.113066 doi: 10.1016/j.na.2022.113066
    [18] G. Stampacchia, Le problème de Dirichlet pour les équations elliptiques du second ordre à coefficients discontinus, Ann. Inst. Fourier, 15 (1965), 189–257. https://doi.org/10.5802/aif.204 doi: 10.5802/aif.204
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