Caccioppoli-type estimates for a class of nonlinear differential operators

We establish Caccioppoli-type estimates for a class of nonlinear differential equations with the aid of a differential identity that generalizes the well-known multidimensional Picone’s formula. In special cases, these estimates give the Finsler $p$-Laplacian, the $p$-Laplacian and the pseudo-$p$-La...

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Date:2018
Main Authors: Tiryaki, A., Тирякі, А.
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Language:English
Published: Institute of Mathematics, NAS of Ukraine 2018
Online Access:https://umj.imath.kiev.ua/index.php/umj/article/view/1646
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Journal Title:Ukrains’kyi Matematychnyi Zhurnal
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Ukrains’kyi Matematychnyi Zhurnal
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author Tiryaki, A.
Тирякі, А.
author_facet Tiryaki, A.
Тирякі, А.
author_sort Tiryaki, A.
baseUrl_str https://umj.imath.kiev.ua/index.php/umj/oai
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datestamp_date 2019-12-05T09:21:55Z
description We establish Caccioppoli-type estimates for a class of nonlinear differential equations with the aid of a differential identity that generalizes the well-known multidimensional Picone’s formula. In special cases, these estimates give the Finsler $p$-Laplacian, the $p$-Laplacian and the pseudo-$p$-Laplacian.
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fulltext UDC 517.9 A. Tiryaki (Izmir Univ., Turkey) CACCIOPPOLI-TYPE ESTIMATES FOR A CLASS OF NONLINEAR DIFFERENTIAL OPERATORS ОЦIНКИ ТИПУ КАЧЧIОППОЛI ДЛЯ ОДНОГО КЛАСУ НЕЛIНIЙНИХ ДИФЕРЕНЦIАЛЬНИХ РIВНЯНЬ We establish Caccioppoli-type estimates for a class of nonlinear differential equations with the aid of a differential identity that generalizes the well-known multidimensional Picone’s formula. In special cases, these estimates give the Finsler p-Laplacian, the p-Laplacian and the pseudo-p-Laplacian. Встановлено оцiнки типу Каччiопполi для одного класу нелiнiйних диференцiальних рiвнянь за допомогою дифе- ренцiальної тотожностi, що узагальнює вiдому багатовимiрну формулу Пiконе. В частинних випадках цi оцiнки дають p-лапласiан Фiнслера, p-лапласiан та p-псевдолапласiан. 1. Introduction. The Caccioppoli inequality is an important tool for the regularity estimate of elliptic partial differential equations (see [1, 2] and references therein). In the basic Caccioppoli inequality, L2-norm of the gradient of a harmonic (or subharmonic) function v is estimated in terms of the L2-norm of v itself. Such an estimate may not hold for arbitrary functions v, but we can typically use them for solutions of elliptic equations or systems in which integrals of higher derivatives can be bounded in terms of integrals of lower derivatives, usually over a slightly larger set. One of the alternative ways to establish the basic Caccioppoli inequality is to derive it from Picone’s identity [3, 4]: \bigm\| \bigm\| \nabla u \bigm\| \bigm\| 2 2 - \biggl\langle \nabla \biggl( u2 v \biggr) ,\nabla v \biggr\rangle = \bigm\| \bigm\| \bigm\| \nabla u - u v \nabla v \bigm\| \bigm\| \bigm\| 2 2 , (1.1) where u and v are differentiable functions in a domain \Omega \subset Rn, v(x) \not = 0 in \Omega , \| \cdot \| 2, \nabla and \langle , \rangle denote the Euclidean norm, the usual gradient and the inner product in Rn, respectively. Let v > 0 be a weak (continuous) solution of \bigtriangleup v = 0 in \Omega and \eta \in C\infty 0 (\Omega ) be a nonnegative test function. If we integrate (1.1) by substituting u = \eta v, and use Young’s inequality and Cauchy – Schwartz inequality, respectively, then we can obtain the desired estimate\int \Omega \bigm\| \bigm\| \eta \nabla v \bigm\| \bigm\| 2 2 dx \leq 4 \int \Omega \bigm\| \bigm\| v\nabla \eta \bigm\| \bigm\| 2 2 dx. More generally, if p > 1 is fixed and v > 0 is a weak continuous solution (or subsolution) of the p-harmonic equation \mathrm{d}\mathrm{i}\mathrm{v} \bigl( \| \nabla v\| p - 2 2 \nabla v \bigr) = 0 in \Omega , c\bigcirc A. TIRYAKI, 2018 ISSN 1027-3190. Укр. мат. журн., 2018, т. 70, № 10 1429 1430 A. TIRYAKI then the Lp-version of the Caccioppoli estimate\int \Omega \bigm\| \bigm\| \eta \nabla v \bigm\| \bigm\| p 2 dx \leq pp \int \Omega \bigm\| \bigm\| v\nabla \eta \bigm\| \bigm\| p 2 dx ([5], see also inequality (5.27) in [6] and Corollary A6 in [7]) can be easily obtained from the p-Laplacian generalization of Picone’s identity \bigm\| \bigm\| \nabla u \bigm\| \bigm\| p 2 - \biggl\langle \nabla \biggl( | u| p vp - 1 \biggr) , \bigm\| \bigm\| \nabla v \bigm\| \bigm\| p - 2 2 \nabla v \biggr\rangle = \Phi p(u, v), where \Phi p(u, v) := \bigm\| \bigm\| \nabla u \bigm\| \bigm\| p 2 + (p - 1) \| u\| p vp \| \nabla v\| p2 - p | u| p - 1 vp - 1 \Bigl\langle \nabla u, \| \nabla v\| p - 2 2 \nabla v \Bigr\rangle \geq 0 by setting u = \eta v and making use of Young’s and Hölder inequality [8, 9]. Recently, Jaroš [10] extended the Caccioppoli inequality to a class of differential operators of the form \Delta H,pv := \mathrm{d}\mathrm{i}\mathrm{v} \bigl( H(\nabla v)p - 1\nabla \xi H(\nabla v) \bigr) , (1.2) where p > 1, H : Rn \rightarrow [0,\infty ), n \geq 2 is a convex function (see, for example, [11]) of the class C1(Rn\setminus \{ 0\} ) which is positively homogeneous of degree 1 and \nabla and \nabla \xi stand for usual gradient operators with respect to the variables x and \xi , respectively. We refer to the operator \Delta H,p as the Finsler p-Laplacian (or the anisotropic p-Laplacian). A prototype of H satisfying the above conditions is the lr -norm H(\xi ) = \| \xi \| r = \Biggl( n\sum i=1 | \xi i| r \Biggr) 1/r , r > 1, for which the operator defined by (1.2) has the form \Delta r,pv := \mathrm{d}\mathrm{i}\mathrm{v} \bigl( \| \nabla v\| p - r r \nabla rv \bigr) , (1.3) where \nabla rv := \Biggl( \bigm| \bigm| \bigm| \bigm| \partial v\partial x1 \bigm| \bigm| \bigm| \bigm| r - 2 \partial v \partial x1 , . . . , \bigm| \bigm| \bigm| \bigm| \partial v\partial xn \bigm| \bigm| \bigm| \bigm| r - 2 \partial v \partial xn \Biggr) . (1.4) The class of operators of the form (1.3) includes the usual p-Laplacian and the so-called pseudo- p-Laplace operator as the special cases corresponding to r = 2 and p \in (1,\infty ) and r = p > 1, respectively. Clearly, if p = r = 2, then (1.3) reduces to the standard Laplacian \Delta . Anisotropic elliptic problems involving this kind of operator have recently been studied in several papers including [6, 12 – 22]. Recently, Jaroš obtained the following interesting result related to Caccioppoli inequality: ISSN 1027-3190. Укр. мат. журн., 2018, т. 70, № 10 CACCIOPPOLI-TYPE ESTIMATES FOR A CLASS OF NONLINEAR DIFFERENTIAL OPERATORS 1431 Theorem 1.1 (Caccioppoli-type inequality) [10]. Let v > 0 be a weak subsolution of - \Delta H,pv = g(x)| v| p - 2v in \Omega . Then, for any fixed q > p - 1 and w = vq/p, the inequality\int \Omega H(\eta \nabla w)pdx \leq \biggl( q q - p+ 1 \biggr) p \int \Omega H(w\nabla \eta )pdx+ qpp1 - p q - p+ 1 \int \Omega g(x)wp\eta pdx (1.5) holds for all 0 \leq \eta \in C\infty 0 (\Omega ), where 0 \leq g \in L\infty Loc(\Omega ). The purpose of this paper is to extend the Caccioppoli inequality to a class of A-harmonic operators of the form \Delta Av := \mathrm{d}\mathrm{i}\mathrm{v} \bigl( \nabla \xi A(x,\nabla v) \bigr) , (1.6) where A : \Omega \times Rn \rightarrow R+ is measurable function such that \xi \rightarrow A(x, \xi ) is continuously differentiable function, convex and homogeneous of degree p > 1 with A(x, \xi ) \leq A1(x)A2(\xi ). A typical example of functions A satisfying the above hypothesis is A(x, \xi ) = 1 p \| \xi \| pr , p > 1, r > 1, \xi \in Rn, or more generally A(x, \xi ) = 1 p H(\xi )p, p > 1. In these two important particular cases, (1.6) reduces to (1.3) and (1.2), respectively. 2. Preliminaries. In this section we give some properties of the A-harmonic operator and general norms in Rn which will be used in the sequel. The proofs can be obtained similarly as in [15] or [16]. Let \langle , \rangle denote the usual inner product in Rn and A : \Omega \times Rn \rightarrow R+ be a measurable function such that \xi \rightarrow A(x, \xi ) is convex and homogeneous of degree p > 1 so that A(x, t\xi ) = | t| pA(x, \xi ) (2.1) for all t \in R and (x, \xi ) \in \Omega \times Rn. If we assume that A \in C1(\Omega \times Rn\setminus \{ 0\} ), then from (2.1) it follows that \langle \xi ,\nabla \xi A(x, t\xi )\rangle = pA(x, \xi ) for all (x, \xi ) \in \Omega \times Rn [23]. Let A2 be an arbitrary norm in Rn. If we define the dual norm A0 of A2 by A0(u) = p - 1 p \mathrm{s}\mathrm{u}\mathrm{p} \langle u, \xi \rangle A2(\xi ) 1 p for u \in Rn ISSN 1027-3190. Укр. мат. журн., 2018, т. 70, № 10 1432 A. TIRYAKI and if we assume A2 \in C1 \bigl( Rn\setminus \{ 0\} \bigr) , then from (2.1) we obtain \nabla \xi A2(t\xi ) = \mathrm{s}\mathrm{g}\mathrm{n}\mathrm{t} | t| p\nabla \xi A2(\xi ) for all \xi \not = 0 and t \not = 0 (2.2) and \langle \xi ,\nabla \xi A2(\xi )\rangle = pA2(\xi ) for all \xi \in Rn, where the left-hand side is defined to be 0 if \xi = 0. Moreover, A0 \Bigl( \nabla \xi A2(\xi ) 1 p \Bigr) = p - 1 p for all \xi \in Rn\setminus \{ 0\} . Similarly, if A0 is of class C1 for u \not = 0, then A2 \Bigl( \nabla A0(u) 1 p \Bigr) = p - 1 p for all u \in Rn\setminus \{ 0\} . From (2.2), we obtain the Hölder-type inequality \langle u, \xi \rangle \leq p 1 pA0(u)A2(\xi ) 1 p for all u, \xi \in Rn. We will also need the following lemmas. Lemma 2.1 [23]. Let the function \xi \rightarrow A(x, \xi ) be continuously differentiable convex and ho- mogeneous of degree p > 1, that is, A(x, t\xi ) = | t| pA(x, \xi ) for all t \in R and (x, \xi ) \in \Omega \times Rn. Then A(x, \eta ) + (p - 1)A(x, \xi ) \geq \langle \nabla \xi A(x, \xi ), \eta \rangle (2.3) for all \xi , \eta \in Rn. If in addition, \xi \rightarrow A(x, \xi ) is a strictly convex function, then the equality in (2.3) holds if and only if \xi = \eta . Lemma 2.2 (A generalization of Picone’s identity) [23]. Let the function \xi \rightarrow A(x, \xi ) be con- tinuously differentiable convex and homogeneous of degree p > 1. Assume that u and v are differen- tiable in a given domain \Omega \subset Rn with v(x) \not = 0 in \Omega and denote \Phi A(u, v) := A(x,\nabla u) + (p - 1)A \Bigl( x, u v \nabla v \Bigr) - \Bigl\langle \nabla \xi A \Bigl( x, u v \nabla v \Bigr) ,\nabla u \Bigr\rangle . Then A(x,\nabla u) - 1 p \biggl\langle \nabla \xi A(x,\nabla v),\nabla \biggl( | u| p | v| p - 2v \biggr) \biggr\rangle = \Phi A(u, v) (2.4) and \Phi A(u, v) \geq 0 a.e. in \Omega . If , in addition, the function \xi \rightarrow A(x, \xi ) is strictly convex in Rn, then \Phi A(u, v) = 0 a.e. in \Omega if and only if u\nabla v = v\nabla u in \Omega . Remark 2.1. In the special case, where A(x, \xi ) = 1 p H(\xi )p, p > 1, Lemmas 2.1 and 2.2 reduce to Lemmas 2.1 and 2.2 in [10], respectively. In [10], this special formula was used to establish the Caccioppoli-type inequality (1.5) for the subsolution (resp. the supersolution) of the nonlinear equation involving a Finsler p-Laplace operator \bigtriangleup H,p. Similarly in the special case, where A(x, \xi ) = = 1 p \| \xi \| pr , where p, r > 1, \xi \in Rn, the identity (2.4) reduces to ISSN 1027-3190. Укр. мат. журн., 2018, т. 70, № 10 CACCIOPPOLI-TYPE ESTIMATES FOR A CLASS OF NONLINEAR DIFFERENTIAL OPERATORS 1433 \| \nabla u\| pr - \biggl\langle \nabla \biggl( | u| p | v| p - 2v \biggr) , \| \nabla v\| p - r r \nabla rv \biggr\rangle = \Phi p,r(u, v), where \nabla rv is defined in (1.4) and \Phi p,r(u, v) := \| \nabla u\| pr + (p - 1) | u| p | v| p \| \nabla v\| pr - p | u| p - 2u | v| p - 2v \bigl\langle \nabla u, \| \nabla v\| p - 2 r \nabla rv \bigr\rangle \geq 0 which is the special case of (2.4). 3. Caccioppoli-type estimates. In this section we establish Caccioppoli-type estimates for positive sub- and supersolutions of nonlinear equations involving anisotropic elliptic operators \bigtriangleup A where A(x, \xi ) \leq A1(x)A2(\xi ). Let \Omega be a domain in Rn and A : \Omega \times Rn \rightarrow [0,\infty ) be a special Caratheodory function, i.e., A1 \in C(\Omega ) with A1(x) > 0, A2 is measurable nonnegative function for all \xi \in Rn. Moreover we assume that A2(\xi ) is differentiable and satisfies the properties given in Section 2. Consider the equation - 1 p \bigtriangleup Av = g(x)| v| p - 2v + f(x), (3.1) where p > 1, 0 \leq g \in L\infty (\Omega ), 0 \leq f \in Lp\prime (\Omega ) and p\prime = p - 1 p . As usual we will say that a continuous function v \in W 1,p(\Omega ) is a (weak) solution of Eq. (3.1) in a domain \Omega \subset Rn if it satisfies 1 p \int \Omega \bigl\langle \nabla \xi A(x,\nabla u),\nabla \eta \bigr\rangle dx - \int \Omega g(x)| v| p - 2v\eta dx = \int \Omega f(x)\eta dx (3.2) for all \eta \in W 1,p 0 (\Omega ). (Weak) subsolution and supersolution (3.1) are defined analogously using the nonnegative test functions \eta \in W 1,p 0 (\Omega ) by replacing `` = "" in (3.2) with `` \leq "" and `` \geq "", respectively. We define the functional JA as JA(u; \Omega ) := \int \Omega A(x,\nabla u)dx - \int \Omega g(x)| u| pdx, u \in W 1,p 0 (\Omega ) associated with (3.1). Let v > 0 be a (continuous) weak subsolution of (3.1) in \Omega and u \in W 1,p 0 (\Omega ). Then we can choose \eta = | u| p vp - 1 as a test function in (3.1) and conclude by (2.4), that JA(u; \Omega ) \leq \int \Omega \biggl\{ A(x,\nabla u) - 1 p \biggl\langle \nabla \xi A(x,\nabla u),\nabla \biggl( | u| p vp - 1 \biggr) \biggr\rangle \biggr\} dx+ \int \Omega f(x) | u| p vp - 1 dx = = \int \Omega \Phi A(u, v)dx+ \int \Omega f(x) | u| p vp - 1 dx. (3.3) ISSN 1027-3190. Укр. мат. журн., 2018, т. 70, № 10 1434 A. TIRYAKI Clearly, for positive supersolution v of (3.1) and any u \in W 1,p 0 (\Omega ), the reversed inequality JA(u; \Omega ) \geq \int \Omega \Phi A(u, v)dx+ \int \Omega f(x) | u| p vp - 1 dx. holds true. If, in particular, v \in W 1,p 0 (\Omega ) is a positive solution of (3.1), then (3.3) becomes an equality. Then we have the following theorem. Theorem 3.1 (Caccioppoli-type inequality). Let v > 0 be weak subsolution of (3.1) in \Omega . Then for any fixed q > p - 1 and w = v q p , the inequality qp q - p+ 1 \int \Omega A(x, \eta \nabla w)dx - (p - 1)(q + 1) q - p+ 1 \int \Omega A1(x)A2(\eta \nabla w)dx \leq \leq \biggl( q q - p+ 1 \biggr) p \int \Omega A1(x)A2(w\nabla \eta )dx+ qpp1 - p q - p+ 1 \int \Omega g(x)wp\eta pdx+ qpp1 - p q - p+ 1 \int \Omega f(x)\eta dx (3.4) holds for all 0 \leq \eta \in C\infty 0 (\Omega ). Proof. Let v be a positive subsolution of (3.1) in \Omega . Fix a nonnegative function \eta \in C\infty 0 (\Omega ). Then u := v q p \eta belongs to W 1,p 0 (\Omega ) and we can use it as a test function in (3.3) to get JA(v q p \eta ; \Omega ) \leq \int \Omega A(x,\nabla v q p \eta )dx+ (p - 1) \int \Omega A \Bigl( x, v q - p p \eta \nabla v \Bigr) dx - - \int \Omega \Bigl\langle \nabla \xi A \bigl( x, v q - p p \eta \nabla v \bigr) ,\nabla \bigl( v q p \eta \bigr) \Bigr\rangle dx+ \int \Omega f(x)\eta dx. (3.5) By using \nabla \bigl( v q p \eta \bigr) = q p v q p - 1 \eta \nabla v + v q p\nabla \eta and A(x, \xi ) \leq A1(x)A2(\xi ) in the above inequality (3.5), we have JA \bigl( v q p \eta ; \Omega \bigr) \leq \int \Omega A \bigl( x,\nabla v q p \eta \bigr) dx+ (p - 1) \int \Omega A1(x)A2(v q - p p \eta \nabla v)dx - - \int \Omega \biggl\langle \nabla \xi A \bigl( x, v q - p p \eta \nabla v \bigr) , q p v q - p p \eta \nabla v \biggr\rangle dx+ + \int \Omega \Bigl\langle \nabla \xi A1(x)A2 \bigl( v q - p p \eta \nabla v \bigr) , v q p\nabla \eta \Bigr\rangle dx+ \int \Omega f(x)\eta dx. (3.6) ISSN 1027-3190. Укр. мат. журн., 2018, т. 70, № 10 CACCIOPPOLI-TYPE ESTIMATES FOR A CLASS OF NONLINEAR DIFFERENTIAL OPERATORS 1435 On the other hand by using properties of A0 and A2, we can easily obtain\Bigl\langle \nabla \xi A1(x)A2(v q - p p \eta \nabla v), v q p\nabla \eta \Bigr\rangle = A1(x) \Bigl\langle \nabla \xi \Bigl[ A2(v q - p p \eta \nabla v) 1 p \Bigr] p , v q p\nabla \eta \Bigr\rangle \leq \leq pA1(x)A2 \bigl( v q - p p \eta \nabla v \bigr) p - 1 p A2 \bigl( v q p\nabla \eta \bigr) 1 p . By using this inequality in (3.6), we get JA(v q p \eta ; \Omega ) \leq \int \Omega A \bigl( x,\nabla v q p \eta \bigr) dx - - (1 - p) \int \Omega A1(x)A2 \bigl( v q - p p \eta \nabla v \bigr) dx - q \int \Omega A \bigl( x, v q - p p \eta \nabla v \bigr) dx+ +p \int \Omega A1(x)A2 \bigl( v q - p p \eta \nabla v \bigr) p - 1 p A2(v q p\nabla \eta ) 1 pdx+ \int \Omega f(x)\eta dx. Applying Young’s inequality in the form a 1 p bp - 1 \leq 1 p 1 \tau p - 1 a+ p - 1 p \tau bp, a, b \geq 0, \tau > 0, we have JA(v q p \eta ; \Omega ) \leq \int \Omega A \bigl( x,\nabla v q p \eta \bigr) dx - - \bigl[ 1 - p+ (1 - p)\tau \bigr] \int \Omega A1(x)A2 \bigl( v q - p p \eta \nabla v \bigr) dx - q \int \Omega A \bigl( x, v q - p p \eta \nabla v \bigr) dx+ + 1 \tau p - 1 \int \Omega A1(x)A2 \bigl( v q p\nabla \eta \bigr) dx+ \int \Omega f(x)\eta dx. Now making use of the definition of JA we obtain q \int \Omega A \bigl( x, v q - p p \eta \nabla v \bigr) dx \leq (p - 1)(1 + \tau ) \int \Omega A1(x)A2 \bigl( v q - p p \eta \nabla v \bigr) dx+ + 1 \tau p - 1 \int \Omega A1(x)A2 \bigl( v q p\nabla \eta \bigr) dx \int \Omega g(x)vq\eta pdx+ \int \Omega f(x)\eta dx, which after choosing the constant \tau := q - p+ 1 p as in [10], leads to qp q - p+ 1 \int \Omega A \bigl( x, v q - p p \eta \nabla v \bigr) dx - (p - 1)(q + 1) q - p+ 1 \int \Omega A1(x)A2 \bigl( v q - p p \eta \nabla v \bigr) dx \leq ISSN 1027-3190. Укр. мат. журн., 2018, т. 70, № 10 1436 A. TIRYAKI \leq \biggl( p q - p+ 1 \biggr) p \int \Omega A1(x)A2 \bigl( v q p\nabla \eta \bigr) dx+ + p q - p+ 1 \int \Omega g(x)vq\eta pdx+ p q - p+ 1 \int \Omega f(x)\eta dx. Finally, the substitution of w = v q p yields (3.4) as claimed. Theorem 3.1 is proved. An analogous result as Theorem 3.1 above holds for positive supersolution of (3.1) and a range of q smaller than p - 1. The proof is similar to that of Theorem 3.1, hence omitted. Theorem 3.2. Let v > 0 be a weak supersolution of (3.1) in \Omega . Then, for any fixed q < p - 1, the inequality (p - 1)(q + 1) p - q - 1 \int \Omega A1(x)A2 \bigl( v q - p p \eta \nabla v \bigr) dx - qp p - q - 1 \int \Omega A(x, v q - p p \eta \nabla v)dx \leq \leq \biggl( p p - q - 1 \biggr) p \int \Omega A1(x)A2(v q p\nabla \eta )dx - - p p - q - 1 \int \Omega g(x)vq\eta pdx - p p - q - 1 \int \Omega f(x)\eta dx (3.7) holds for all \eta \in C\infty 0 (\Omega ) with \eta \geq 0. Now we consider the equality case, that is, A(x, \xi ) = A1(x)A2(\xi ). From Theorems 3.1 and 3.2 we have the following results. Theorem 3.3 (Caccioppoli-type inequality). Let v > 0 be weak subsolution of (3.1) in \Omega . Then, for any fixed q > p - 1 and w = v q p , the inequality\int \Omega A1(x)A2(\eta \nabla w)dx \leq \biggl( q q - p+ 1 \biggr) p \int \Omega A1(x)A2(w\nabla \eta )dx+ + qpp1 - p q - p+ 1 \int \Omega g(x)wp\eta pdx+ qpp1 - p q - p+ 1 \int \Omega f(x)\eta dx holds for all 0 \leq \eta \in C\infty 0 (\Omega ). Corollary 3.1. Let q = p, g(x) \equiv 0, and f(x) \equiv 0 in \Omega . If v > 0 is a weak subsolution of (3.1) in \Omega , then \int \Omega A1(x)A2(\eta \nabla v)dx \leq pp \int \Omega A1(x)A2(v\nabla \eta )dx for any nonnegative \eta \in C\infty 0 (\Omega ). ISSN 1027-3190. Укр. мат. журн., 2018, т. 70, № 10 CACCIOPPOLI-TYPE ESTIMATES FOR A CLASS OF NONLINEAR DIFFERENTIAL OPERATORS 1437 Theorem 3.4. Let r > 0 be a weak supersolution of (3.1) in \Omega . Then, for any fixed q < p - 1, the inequality \int \Omega A1(x)A2 \bigl( v q p - 1 \eta \nabla v \bigr) dx \leq \biggl( p p - q - 1 \biggr) p \int \Omega A1(x)A2 \bigl( v q p\nabla \eta \bigr) dx - - p p - q - 1 \int \Omega g(x)vq\eta pdx - p p - q - 1 \int \Omega f(x)\eta dx holds for all \eta \in C\infty 0 (\Omega ) with \eta \geq 0. The particular case of the above theorem when q = 0 is interesting in the sense that the right-hand side of (3.7) does not contain v. The result specializes as follows. Corollary 3.2 (Logarithmic Caccioppoli-type inequality). Let v > 0 be weak subsolution of (3.1) in \Omega . Then \int \Omega A1(x)A2(\eta \nabla logv)dx \leq \biggl( p p - 1 \biggr) p \int \Omega A1(x)A2(\nabla \eta )dx - - p p - 1 \int \Omega g(x)\eta pdx - p p - 1 \int \Omega f(x)\eta dx (3.8) whenever 0 \leq \eta \in C\infty 0 (\Omega ). If A(\xi ) = 1 p \| \xi \| p2, p > 1, \xi \in Rn, and g(x) \equiv 0 and f(x) \equiv 0 in \Omega , then (3.8) reduces to the well-known logarithmic Caccioppoli inequality for the positive p-superharmonic functions [24]. References 1. Gariepy R. F. A Caccioppoli inequality and partial regularity in the calculus of variations // Proc. Roy. Soc. Edinburgh Sect. A. – 1989. – 112, №. 3-4. – P. 249 – 255. 2. Giaquinta M. Multiple integrals in the calculus of variations and nonlinear elliptic sytsems. – Princeton Univ. Press, 1983. 3. Picone M. Un teorema sulle soluzioni delle equazioni lineari ellittiche autoaggiunte alle derivate parziali del secondo- ordine // Atti Accad. Naz. Lincei Rend. – 1911. – 20. – P. 213 – 219. 4. Swanson Charles A. Picones identity // Rend. Mat. – 1975. – 8, №. 2. – P. 373 – 397. 5. Iwaniec T., Sbordone C. Caccioppoli estimates and very weak solutions of elliptic equations // Atti Accad. Naz. Lincei Cl. Sci. Fis. Mat. Natur. – 2003. – 14, №. 3. – P. 189 – 205. 6. 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Existence and nonexistence results for quasilinear elliptic equations involving the p- Laplacian with a critical potential // Ann. Mat. Pura ed Appl. – 2003. – 182, №. 3. – P. 247 – 270. ISSN 1027-3190. Укр. мат. журн., 2018, т. 70, № 10 1438 A. TIRYAKI 13. Alvino A., Ferone V., Trombetti G„ Lions P.-L. Convex symmetrization and applications // Ann. Inst. H. Poincaré Anal. Non Linéaire. – 1997. – 14, №. 2. – P. 275 – 293. 14. Belloni M., Ferone V., Kawohl B. Isoperimetric inequalities, Wulff shape and related questions for strongly nonlinear elliptic operators // Z. angew. und math. Phys. – 2003. – 54, №. 5. – S. 771 – 783. 15. Bellettini G., Paolini M. Anisotropic motion by mean curvature in the context of Finsler geometry // Hokkaido Math. J. – 1996. – 25, №. 3. – P. 537 – 566. 16. Cianchi A., Salani P. Overdetermined anisotropic elliptic problems // Math. Ann. – 2009. – 345, №. 4. – P. 859 – 881. 17. Francesco D. P., Nunzia G. 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Lewis J., Lindqvist P., Manfredi J. J., Salsa S. Regularity estimates for nonlinear elliptic and parabolic problems // Lect. Notes Math. – 2012. – 2045. Received 16.03.16 ISSN 1027-3190. Укр. мат. журн., 2018, т. 70, № 10
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spelling umjimathkievua-article-16462019-12-05T09:21:55Z Caccioppoli-type estimates for a class of nonlinear differential operators Оцiнки типу Каччiопполi для одного класу нелiнiйних диференцiальних рiвнянь Tiryaki, A. Тирякі, А. We establish Caccioppoli-type estimates for a class of nonlinear differential equations with the aid of a differential identity that generalizes the well-known multidimensional Picone’s formula. In special cases, these estimates give the Finsler $p$-Laplacian, the $p$-Laplacian and the pseudo-$p$-Laplacian. Встановлено оцiнки типу Каччiопполi для одного класу нелiнiйних диференцiальних рiвнянь за допомогою диференцiальної тотожностi, що узагальнює вiдому багатовимiрну формулу Пiконе. В частинних випадках цi оцiнки дають $p$-лапласiан Фiнслера, $p$-лапласiан та $p$-псевдолапласiан. Institute of Mathematics, NAS of Ukraine 2018-10-25 Article Article application/pdf https://umj.imath.kiev.ua/index.php/umj/article/view/1646 Ukrains’kyi Matematychnyi Zhurnal; Vol. 70 No. 10 (2018); 1429-1438 Український математичний журнал; Том 70 № 10 (2018); 1429-1438 1027-3190 en https://umj.imath.kiev.ua/index.php/umj/article/view/1646/628 Copyright (c) 2018 Tiryaki A.
spellingShingle Tiryaki, A.
Тирякі, А.
Caccioppoli-type estimates for a class of nonlinear differential operators
title Caccioppoli-type estimates for a class of nonlinear differential operators
title_alt Оцiнки типу Каччiопполi для одного класу нелiнiйних диференцiальних рiвнянь
title_full Caccioppoli-type estimates for a class of nonlinear differential operators
title_fullStr Caccioppoli-type estimates for a class of nonlinear differential operators
title_full_unstemmed Caccioppoli-type estimates for a class of nonlinear differential operators
title_short Caccioppoli-type estimates for a class of nonlinear differential operators
title_sort caccioppoli-type estimates for a class of nonlinear differential operators
url https://umj.imath.kiev.ua/index.php/umj/article/view/1646
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AT tirâkía caccioppolitypeestimatesforaclassofnonlineardifferentialoperators
AT tiryakia ocinkitipukaččioppolidlâodnogoklasunelinijnihdiferencialʹnihrivnânʹ
AT tirâkía ocinkitipukaččioppolidlâodnogoklasunelinijnihdiferencialʹnihrivnânʹ