Generalized Picone identity for Finsler $p$-Laplacian and its applications

UDC 517.9 We prove a generalized Picone-type identity for Finsler $p$-Laplacian and use it to establish some qualitative results for some boundary-value problems involving Finsler $p$-Laplacian.  

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Datum:2021
1. Verfasser: Dwivedi, G.
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Veröffentlicht: Institute of Mathematics, NAS of Ukraine 2021
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Ukrains’kyi Matematychnyi Zhurnal
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author Dwivedi, G.
Dwivedi, G.
author_facet Dwivedi, G.
Dwivedi, G.
author_sort Dwivedi, G.
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description UDC 517.9 We prove a generalized Picone-type identity for Finsler $p$-Laplacian and use it to establish some qualitative results for some boundary-value problems involving Finsler $p$-Laplacian.  
doi_str_mv 10.37863/umzh.v73i11.1050
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fulltext DOI: 10.37863/umzh.v73i11.1050 UDC 517.9 G. Dwivedi (Birla Inst. Technology and Sci. Pilani, Rajasthan, India) GENERALIZED PICONE IDENTITY FOR FINSLER \bfitp -LAPLACIAN AND ITS APPLICATIONS* УЗАГАЛЬНЕНА ТОТОЖНIСТЬ ПIКОНЕ ДЛЯ \bfitp -ЛАПЛАСIАНА ФIНСЛЕРА ТА ЇЇ ЗАСТОСУВАННЯ We prove a generalized Picone-type identity for Finsler p-Laplacian and use it to establish some qualitative results for some boundary-value problems involving Finsler p-Laplacian. Доведено узагальнену тотожнiсть типу Пiконе для p-лапласiана Фiнслера, яку потiм використано для отримання деяких якiсних результатiв для граничних задач, що включають p-лапласiан Фiнслера. 1. Introduction. In this paper, we establish a generalized Picone identity for the class of operators \Delta H,pu := \mathrm{d}\mathrm{i}\mathrm{v}(H(\nabla u)p - 1\nabla \xi H(\nabla u)), (1.1) where p > 1, H : \BbbR n \rightarrow [0,\infty ), n \geq 2, is a strictly convex, twice differentiable function which is positively homogeneous of degree 1, \Delta and \Delta \xi denote the usual gradient operators with respect to variable x and \xi , respectively. The operators of the form (1.1) are called Finsler p-Laplacian or anisotropic p-Laplacian. A prototype function H is given by H(\xi ) = \| \xi \| r = \Biggl( n\sum i=1 | \xi i| r \Biggr) 1/r , r > 1. For this choice of H, the operator (1.1) reduces to \Delta H,pv = \mathrm{d}\mathrm{i}\mathrm{v} \bigl( \| \nabla v\| p - 2 r \nabla rv \bigr) , (1.2) where \nabla rv = \bigl( | vx1 | r - 2vx1 , . . . , | vxn | r - 2vxn \bigr) . (1.2) reduces to p-Laplacian if r = 2 and p \in (1,\infty ), while it reduces to pseudo p-Laplacian if r = p > 1. In case of r = p = 2, we get standard Laplace operator from (1.2). Finsler p-Laplacian has been studied by several authors. V. Ferone and B. Kawohl [18] proved some properties of Finsler p-Laplacian such as existence of fundamental solution, maximum prin- ciple, comparison principle, mean value property etc. Belloni et al. [6] obtained positivity and simplicity of the first eigenvalue and Faber – Krahn inequality for Finsler p-Laplacian with Dirichlet boundary conditions. They also established symmetry of positive solutions to - \Delta H,nu = f(u) in \Omega , u = 0 on \partial \Omega , where \Omega is a smooth and bounded domain in \BbbR n. G. Wang and C. Xia [26] obtained a lower bound for the first eigenvalue for Finsler p-Laplacian with Neumann boundary conditions. F. Della Pietra and * This paper was supported by Science and Engineering Research Board, India (the grant MTR/2018/000233). c\bigcirc G. DWIVEDI, 2021 ISSN 1027-3190. Укр. мат. журн., 2021, т. 73, № 11 1451 1452 G. DWIVEDI N. Gavitone [9, 10] discussed existence and properties of the first eigenvalue of Finsler p-Laplacian with Dirichlet and Robin boundary conditions. G. Wang and C. Xia [27] studied blow up analysis for the problem - \Delta H,2u = V (x)eu in dimension 2. We refer to [8, 22, 24, 29] and reference cited therein for some further existence and qualitative results involving Finsler p-Laplacian. Next, let us recall some historical developments in Picone identity. The classical Picone iden- tity [23] says that if u and v are differentiable functions such that v > 0 and u \geq 0, then | \nabla u| 2 + u2 v2 | \nabla v| 2 - 2 u v \nabla u\nabla v = | \nabla u| 2 - \nabla \biggl( u2 v \biggr) \nabla v \geq 0. (1.3) (1.3) has an enormous applications to second-order elliptic equations and systems (see, for instance, [1, 2, 21] and the references therein). In order to apply (1.3) to p-Laplace equations, W. Allegretto and Y. X. Huang [3] extended (1.3) as follows. Theorem 1.1 [3]. Let v > 0 and u \geq 0 be differentiable functions in a domain \Omega of \BbbR n. Denote L(u, v) = | \nabla u| p + (p - 1) up vp | \nabla v| p - p up - 1 vp - 1 | \nabla v| p - 2\nabla u\nabla v, R(u, v) = | \nabla u| p - \nabla \biggl( up vp - 1 \biggr) | \nabla v| p - 2\nabla v. Then L(u, v) = R(u, v). Moreover, L(u, v) \geq 0 and L(u, v) = 0 a.e. in \Omega if and only if \nabla \Bigl( u v \Bigr) = 0 a.e. in \Omega . A nonlinear analogue of Theorem 1.1 was proved by J. Tyagi [25] in case of p = 2 and by K. Bal [4] in general case. The results of K. Bal [4] was further generalized by T. Feng [16] as follows. Theorem 1.2 [16]. Let v > 0 and u \geq 0 be differentiable functions in a domain \Omega \subseteq \BbbR n, n \geq 3. Assume that differentiable functions g(u) and f(v) satisfy that for p > 1, q > 1, 1 p + 1 q = 1, g(u)f \prime (v)| \nabla v| p [f(v)]2 \geq p q \biggl[ g\prime (u)| \nabla v| p - 1 pf(v) \biggr] q , where g(u), g\prime (u) > 0 for u > 0; g(u), g\prime (u) = 0 for u = 0, and f(v), f \prime (v) > 0. Denote L(u, v) = | \nabla u| p - g\prime (u)| \nabla v| p - 2\nabla v\nabla u f(v) + g(u)f \prime (v)| \nabla v| p [f(v)]2 , R(u, v) = | \nabla u| p - \nabla \biggl( g(u) f(v) \biggr) | \nabla v| p - 2\nabla v. Then L(u, v) = R(u, v) \geq 0. Moreover, L(u, v) = 0 a.e. in \Omega if and only if \nabla \Bigl( u v \Bigr) = 0, | \nabla u| p = \biggl[ g\prime (u)| \nabla v| p - 1 pf(v) \biggr] q , p q \biggl[ g\prime (u)| \nabla v| p - 1 pf(v) \biggr] q = g(u)f \prime (v)| \nabla v| p [f(v)]2 a.e. in \Omega . ISSN 1027-3190. Укр. мат. журн., 2021, т. 73, № 11 GENERALIZED PICONE IDENTITY FOR FINSLER p-LAPLACIAN AND ITS APPLICATIONS 1453 There are several other interesting articles dealing with Picone identity in different contexts. For instance, for a Picone-type identity to higher order half linear differentiable operators, we refer to [20] and the references therein, for Picone identities to half-linear elliptic operators with p(x)-Laplacians, we refer to [28] for Picone-type identity to pseudo p-Laplacian with variable power, we refer to [7] and for Picone identity for biharmonic operators and applications, we refer to [11 – 14, 17]. J. Jaroš [19] proved a Picone identity for the class of operators (1.1). Their main result is follows. Theorem 1.3. Let \Omega \subseteq \BbbR n be a domain and H be an arbitrary norm in \BbbR n which is of class C1 for x \not = 0. Assume that u, v \in W 1,p loc (\Omega ) \cap C(\Omega ) with v(x) \not = 0 in \Omega and denote \Phi (u, v) := H(\nabla u)p + (p - 1) | u| p | v| p H(\nabla v)p - p | u| p - 2u | v| p - 2v \langle \nabla u,H(\nabla v)p - 1\nabla \xi H(\nabla v)\rangle . Then H(\nabla u)p - \biggl\langle \nabla \biggl( | u| p | v| p - 2v \biggr) , H(\nabla v)p - 1\nabla \xi H(\nabla v) \biggr\rangle = \Phi (u, v) and \Phi (u, v) \geq 0 a.e. in \Omega . If , in addition, H(\xi )p is strictly convex in \BbbR n, then \Phi (u, v) = 0 a.e. in \Omega if and only if u is a constant multiple of v in \Omega . Bal et al. [5] generalized Theorem 1.3 as follows. Theorem 1.4. Let \Omega \subseteq \BbbR n be a domain. For u, v \in W 1,p loc (\Omega ) \cap C(\Omega ) with u \geq 0 and v > 0, define A(u, v) = H(\nabla u)p - p up - 1 f(v) \bigl\langle \nabla u,H(\nabla v)p - 1\nabla \xi (\nabla v) \bigr\rangle + upf \prime (v) (f(v))2 H(\nabla v)p = = H(\nabla u)p - \biggl\langle \nabla \biggl( up f(v) \biggr) , H(\nabla v)p - 1\nabla \xi H(\nabla v) \biggr\rangle \geq 0 for f \in \BbbM := \Bigl\{ f : (0,\infty ) \rightarrow (0,\infty )f : f \prime (y) \geq (p - 1)f(y) p - 1 p - 2 \Bigr\} \subset C1((0,\infty )). Moreover, A(u, v) = 0 a.e. in \Omega if and only if u = cv a.e. in \Omega , where c is a constant. In this paper, we prove a new nonlinear Picone-type identity, which is a generalization of Theo- rem 1.4. The main result of this paper is follows. Theorem 1.5. Let H be an arbitrary norm in \BbbR n which is of class C1(\BbbR n\setminus \{ 0\} ). Assume that u, v \in W 1,p loc (\Omega ) \cap C(\Omega ) with u \geq 0 and v > 0, where \Omega \subseteq \BbbR n is a domain. Assume that g and f are twice differentiable functions satisfying g(u)f \prime (v)H(\nabla v)p (f(v))2 \geq p q \biggl( g\prime (u)H(\nabla v)p - 1 pf(v) \biggr) q , where g(u), g\prime (u) > 0 for u > 0, g(u), g\prime (u) = 0 if u = 0, f(v), f \prime (v) > 0. Denote L(u, v) = H(\nabla u)p + g(u)f \prime (v) (f(v))2 H(\nabla v)p - \biggl\langle g\prime (u) f(v) \nabla u,H(\nabla v)p - 1\nabla \xi H(\nabla v) \biggr\rangle , R(u, v) = H(\nabla u)p - \biggl\langle \nabla \biggl( g(u) f(v) \biggr) , H(\nabla v)p - 1\nabla \xi H(\nabla v) \biggr\rangle . Then (i) L(u, v) = R(u, v) \geq 0; (ii) L(u, v) = 0 a.e. in \Omega if and only if ISSN 1027-3190. Укр. мат. журн., 2021, т. 73, № 11 1454 G. DWIVEDI \nabla u = \biggl( g\prime (u) pf(v) \biggr) 1/p - 1 \nabla v, g(u)f \prime (v)H(\nabla v)p (f(v))2 \geq p q \biggl( g\prime (u)H(\nabla v)p - 1 pf(v) \biggr) q , (1.4) H(\nabla u)p = \biggl( g\prime (u)H(\nabla v)p - 1 pf(v) \biggr) q . (1.5) Remark 1.1. 1. If we choose g(u) = up in Theorem 1.5, then we obtain Picone identity of Bal et al. [5]. 2. If we choose g(u) = up and f(v) = vp - 1 in Theorem 1.5, then we obtain Picone identity of J. Jaroš [19]. 3. If we choose H(\xi ) = \Bigl( \sum n i=1 | \xi i| p \Bigr) 1/p in Theorem 1.5, then we obtain Picone identity of T. Feng [16]. This paper is organized as follows. In Section 2, we state some elementary properties of an arbitrary norm. In Section 3, we prove Theorem 1.5 and Section 4 deals with some applications of Theorem 1.5. 2. Preliminaries. In this section, we recall some elementary properties of an arbitrary norm on \BbbR n. For further details, we refer to [19] and references therein. Let H : \BbbR n \rightarrow [0,\infty ) be any arbitrary norm in \BbbR n, i.e., a strictly convex, twice differentiable function such that: (i) H(\xi ) > 0 for any \xi \not = 0, (ii) H(t\xi ) = | t| H(\xi ) for all \xi \in \BbbR n and t \in \BbbR , (iii) if H is C1(\BbbR n\setminus \{ 0\} ), then \nabla \xi H(t\xi ) = sgn t\nabla \xi H(\xi ) for all \xi \not = 0 and t \not = 0, (iv) \langle \xi ,\nabla \xi H(\xi )\rangle = H(\xi ) for all \xi \in \BbbR n, where the left-hand side is zero for \xi = 0, (v) there exist constant 0 < c1 \leq c2 such that c1| x| \leq H(x) \leq c2| x| . Next, we define the dual norm H0 of H by H0(x) = \mathrm{s}\mathrm{u}\mathrm{p} \xi \not =0 \langle x, \xi \rangle H(\xi ) , where \langle \cdot , \cdot \rangle is the usual inner product in \BbbR n. Any norm H of class C1 for \xi \not = 0 and its dual H0 satisfy the following properties: (i) H0(\nabla H(\xi )) = 1 for \xi \in \BbbR n\setminus \{ 0\} , (ii) H(\nabla H0(x)) = 1 for x \in \BbbR n\setminus \{ 0\} , (iii) H[H0(x)\nabla H0(x)]\nabla \xi [H0(x)\nabla H0(x)] = x, (iv) H0[H(\xi )\nabla \xi H(\xi )]\nabla H0[H(\xi )\nabla \xi H(\xi )] = \xi , where (ii), (iii) hold for all x, \xi \in \BbbR n, H(0)\nabla \xi H(0) and H0(0)\nabla H0(0) are defined to be 0. The Hölder-type inequality for norm H as follows: H(\xi )H0(x) \geq \langle x, \xi \rangle , (2.1) and equality holds if and only if H0(x) = H(\eta ). Next, we state an elementary lemma. For a proof we refer to [19]. Lemma 2.1. Let H be a norm in \BbbR n such that H \in C1(\BbbR n\setminus \{ 0\} ) and Hp, 1 < p < \infty , is strictly convex. If H(\xi )p + (p - 1)H(\eta )p - p\langle \xi ,H(\eta )p - 1\nabla H(\eta )\rangle = 0 for some \xi , \eta \in \BbbR n, \eta \not = 0, and H(\xi ) = H(\eta ), then \xi = \eta . ISSN 1027-3190. Укр. мат. журн., 2021, т. 73, № 11 GENERALIZED PICONE IDENTITY FOR FINSLER p-LAPLACIAN AND ITS APPLICATIONS 1455 Lemma 2.2 (Young’s inequality). If a and b are two nonnegative real numbers and p and q are such that 1 p + 1 q = 1, then equality ab \leq ap p + bq q (2.2) holds if and only if ap = bq. Proof. For a proof, we refer to [15]. 3. Proof of Theorem 1.5. It is easy to see that \nabla \biggl( g(u) f(v) \biggr) = f(v)g\prime (u)\nabla u - g(u)f \prime (v)\nabla v (f(v))2 , R(u, v) = H(\nabla u)p - \biggl\langle \nabla \biggl( g(u) f(v) \biggr) , H(\nabla v)p - 1\nabla \xi H(\nabla v) \biggr\rangle = = H(\nabla u)p - \biggl\langle g\prime (u)\nabla u f(v) , H(\nabla v)p - 1\nabla \xi H(\nabla v) \biggr\rangle + \biggl\langle g(u)f \prime (v)\nabla v (f(v))2 , H(\nabla v)p - 1\nabla \xi H(\nabla v) \biggr\rangle = = H(\nabla u)p - \biggl\langle g\prime (u)\nabla u f(v) , H(\nabla v)p - 1\nabla \xi H(\nabla v) \biggr\rangle + g(u)f \prime (v) (f(v))2 H(\nabla v)p = = H(\nabla u)p + g(u)f \prime (v) (f(v))2 H(\nabla v)p - g\prime (u)H(\nabla v)p - 1H(\nabla u) f(v) + g\prime (u)H(\nabla v)p - 1H(\nabla u) f(v) - - \biggl\langle g\prime (u)\nabla u f(v) , H(\nabla v)p - 1\nabla \xi H(\nabla v) \biggr\rangle = = p \biggl[ H(\nabla u)p p + 1 q \biggl( g\prime (u)H(\nabla v)p - 1 pf(v) \biggr) q\biggr] - g\prime (u)H(\nabla v)p - 1H(\nabla u) f(v)\underbrace{} \underbrace{} (I) + + g(u)f \prime (v)H(\nabla v)p (f(v))2 - p q \biggl( g\prime (u)H(\nabla v)p - 1 pf(v) \biggr) q \underbrace{} \underbrace{} (II) + + g\prime (u)H(\nabla v)p - 1H(\nabla u) f(v) - \biggl\langle g\prime (u)\nabla u f(v) , H(\nabla v)p - 1\nabla \xi H(\nabla v) \biggr\rangle \underbrace{} \underbrace{} (III) . Now, we plan to show that (I), (II), (III) are nonnegative. Take a = H(\nabla u) and b = = g\prime (u)H(\nabla v)p - 1 pf(v) in (2.2), we get g\prime (u)H(\nabla v)p - 1H(\nabla u) pf(v) \leq H(\nabla u)p p + 1 q \biggl( g\prime (u)H(\nabla v)p - 1 pf(v) \biggr) q , which implies (I) \geq 0. By using (1.4), we obtain (II) \geq 0. To show (III) \geq 0, let us rewrite ISSN 1027-3190. Укр. мат. журн., 2021, т. 73, № 11 1456 G. DWIVEDI (III) = H(\nabla u)H \Biggl( \biggl( g\prime (u) f(v) \biggr) 1/p - 1 \nabla v \Biggr) p - 1 - - \Biggl\langle \nabla u, H \Biggl( \biggl( g\prime (u) f(v) \biggr) 1/p - 1 \nabla v \Biggr) p - 1 \nabla \xi H \Biggl( \biggl( g\prime (u) f(v) \biggr) 1/p - 1 \nabla v \Biggr) \Biggr\rangle . Take \xi = \nabla u, x = H \Biggl( \biggl( g\prime (u) f(v) \biggr) 1/p - 1 \nabla v \Biggr) p - 1 \nabla \xi H \Biggl( \biggl( g\prime (u) f(v) \biggr) 1/p - 1 \nabla v \Biggr) in (2.1), we obtain \Biggl\langle H \Biggl( \biggl( g\prime (u) f(v) \biggr) 1/p - 1 \nabla v \Biggr) p - 1 \nabla \xi H \Biggl( \biggl( g\prime (u) f(v) \biggr) 1/p - 1 \nabla v \Biggr) ,\nabla u \Biggr\rangle \leq \leq H(\nabla u)H0 \left( H \Biggl( \biggl( g\prime (u) f(v) \biggr) 1/p - 1 \nabla v \Biggr) p - 1 \nabla \xi H \Biggl( \biggl( g\prime (u) f(v) \biggr) 1/p - 1 \nabla v \Biggr) \right) = = H(\nabla u)H \Biggl( \biggl( g\prime (u) f(v) \biggr) 1/p - 1 \nabla v \Biggr) p - 1 = = g\prime (u) f(v) H(\nabla u)H(\nabla v)p - 1 \geq 0. The equality in (I) holds if and only if H(\nabla u)p = \biggl( g\prime (u)H(\nabla v)p - 1 pf(v) \biggr) q = \biggl( g\prime (u) pf(v) \biggr) q H(\nabla v)p, H(\nabla u) = H \Biggl( \biggl( g\prime (u) pf(v) \biggr) 1/p - 1 \nabla v \Biggr) a.e. in \Omega . If \biggl( g\prime (u) pf(v) \biggr) 1/p - 1 \nabla v \not = 0 for some x0 \in S := \{ x \in \Omega : R(u, v) = 0\} , then (I) = H(\nabla u)p + (p - 1) \biggl( g\prime (u) pf(v) \biggr) q H(\nabla v)p - g\prime (u) f(v) H(\nabla v)p - 1H(\nabla u) = = H(\nabla u)p + (p - 1)H \Biggl( \biggl( g\prime (u) pf(v) \biggr) 1/p - 1 \nabla v \Biggr) p - - p \Biggl\langle \nabla u,H \Biggl( \biggl( g\prime (u) pf(v) \biggr) 1/p - 1 \nabla v \Biggr) p - 1 \nabla \xi H \Biggl( \biggl( g\prime (u) pf(v) \biggr) 1/p - 1 \nabla v \Biggr) \Biggr\rangle . When (I) = 0, by Lemma 2.1, \nabla u = \biggl( g\prime (u) pf(v) \biggr) 1/p - 1 \nabla v. ISSN 1027-3190. Укр. мат. журн., 2021, т. 73, № 11 GENERALIZED PICONE IDENTITY FOR FINSLER p-LAPLACIAN AND ITS APPLICATIONS 1457 If \biggl( g\prime (u) pf(v) \biggr) 1/p - 1 \nabla v = 0 for some subset S0 of S, then \nabla u = 0 a.e. in S0 which implies \nabla u = = \biggl( g\prime (u) pf(v) \biggr) 1/p - 1 \nabla v. Theorem 1.5 is proved. 4. Applications of Theorem 1.5. In this section, we use Theorem 1.5 to prove some qualitative result. We assume that \Omega is a smooth and bounded domain in \BbbR n and the functions f and g satisfy assumption of Theorem 1.5. First, we prove a Hardy-type inequality. Theorem 4.1 (Hardy-type inequality). Let \Omega be a bounded domain in \BbbR n and v \in C\infty c (\Omega ) be such that - \Delta H,pv \geq \lambda k(x)f(v), v > 0 in \Omega for some \lambda > 0 and nonnegative function k \in L\infty (\Omega ). Then, for any u \in C\infty c (\Omega ), u \geq 0 and g(u) \in C\infty c (\Omega ), \int \Omega H(\nabla u)pdx \geq \lambda \int \Omega k(x)g(u)dx. Proof. Take \phi \in C\infty c (\Omega ), \phi > 0. By Theorem 1.5, we have 0 \leq \int \Omega L(\phi , v) dx = = \int \Omega R(\phi , v) dx = \int \Omega H(\nabla \phi )pdx - \Delta \biggl( g(\phi ) f(v) \biggr) H(\nabla v)p - 1\nabla \xi H(\nabla v)dx = = \int \Omega H(\nabla \phi )pdx+ \int \Omega g(\phi ) f(v) \Delta H,pv dx \leq \leq \int \Omega H(\nabla \phi )pdx - \lambda \int \Omega g(\phi )k(x) dx, and letting \phi \rightarrow u, we get \int \Omega H(\nabla u)pdx \geq \lambda \int \Omega k(x)g(u)dx. Theorem 4.1 is proved. Next, we prove a comparison result. Theorem 4.2. Let k1(x) and k2(x) be two continuous functions such that k1(x) < k2(x) on a bounded domain \Omega \subset \BbbR n. If there exists a function u \in C2(\Omega ) satisfying - \Delta H,pu = k1(x)g(u) u in \Omega , u > 0, g(u) > 0 in \Omega , u = 0 = g(u) on \partial \Omega , (4.1) ISSN 1027-3190. Укр. мат. журн., 2021, т. 73, № 11 1458 G. DWIVEDI then any nontrivial solution v to the equation - \Delta H,pv = k2(x)f(v) in \Omega (4.2) must change sign. Proof. Assume that v does not change sign and \varepsilon > 0. Since g(u) = 0 on \partial \Omega , g(u) f(v) + \varepsilon \in \in W 1,p 0 (\Omega ). By Theorem 1.5, 0 \leq \int \Omega L(u, v)dx = \int \Omega R(u, v)dx = = \int \Omega H(\nabla u)pdx - \int \Omega \biggl\langle \nabla \biggl( g(u) f(v) + \varepsilon \biggr) , H(\nabla v)p - 1\nabla \xi (\nabla v) \biggr\rangle dx = = \int \Omega H(\nabla u)pdx+ \int \Omega g(u) f(v) + \varepsilon \Delta H,pvdx. As \varepsilon \rightarrow 0, we obtain \int \Omega H(\nabla u)pdx+ \int \Omega g(u) f(v) \Delta H,pvdx \geq 0. (4.3) On using (4.1) and (4.2) in (4.3), we have\int \Omega (k1(x) - k2(x))g(u)dx \geq 0, which is a contradiction because k1(x) < k2(x) and g(u) > 0. Theorem 4.2 is proved. Finally, we establish a qualitative result concerning a system of equations involving Finsler p- Laplacian. Theorem 4.3. Let \Omega be a bounded domain in \BbbR n and (u, v) \in C2(\Omega ) \times C2(\Omega ) be a positive solution to the elliptic system - \Delta H,pu = f(v) in \Omega , - \Delta H,pv = (f(v))2u g(u) in \Omega , u > 0, v > 0, g(u), f(v) > 0 in \Omega , u = 0 = g(u) on \partial \Omega . Then \nabla u = \biggl( g\prime (u) pf(v) \biggr) 1/p - 1 \nabla v. ISSN 1027-3190. Укр. мат. журн., 2021, т. 73, № 11 GENERALIZED PICONE IDENTITY FOR FINSLER p-LAPLACIAN AND ITS APPLICATIONS 1459 Proof. For any \phi 1, \phi 2 \in W 1,p 0 (\Omega ), we get\int \Omega H(\nabla u)p - 1\nabla \xi H(\nabla u)\nabla \phi 1dx = \int \Omega f(v)\phi 1dx, \int \Omega H(\nabla v)p - 1\nabla \xi H(\nabla v)\nabla \phi 2dx = \int \Omega (f(v))2u g(u) \phi 2dx. Let \varepsilon > 0. Since g(u) = 0 on \partial \Omega , g(u) f(v) + \varepsilon \in W 1,p 0 (\Omega ). On choosing \phi 1 = u, \phi 2 = g(u) f(v) + \varepsilon , we obtain \int \Omega H(\nabla u)p - 1\nabla \xi H(\nabla u)\nabla udx = \int \Omega f(v)udx, (4.4) \int \Omega H(\nabla v)p - 1\nabla \xi H(\nabla v)\nabla \biggl( g(u) f(v) + \varepsilon \biggr) dx = \int \Omega uf(v)dx. (4.5) On using (4.4) and (4.5), we have\int \Omega H(\nabla v)p - 1\nabla \xi H(\nabla v)\nabla \biggl( g(u) f(v) + \varepsilon \biggr) dx = \int \Omega uf(v)dx = = \int \Omega H(\nabla u)p - 1\nabla \xi H(\nabla u)\nabla udx = = \int \Omega H(\nabla u)pdx. As \varepsilon \rightarrow 0, we obtain \int \Omega L(u, v)dx = \int \Omega R(u, v)dx = 0 and, by Theorem 1.5, \nabla u = \biggl( g\prime (u) f(v) \biggr) 1/p - 1 a.e. in \Omega . Theorem 4.3 is proved. References 1. W. Allegretto, Positive solutions and spectral properties of weakly coupled elliptic systems, J. Math. Anal. and Appl., 120, № 2, 723 – 729 (1986). 2. W. Allegretto, Sturmian theorems for second order systems, Proc. Amer. Math. 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Zhou, Moser – Trudinger inequality involving the anisotropic Dirichlet norm \bigl( \int \Omega FN (\nabla u)dx \bigr) 1 N on W 1,N 0 (\Omega ), J. Funct. Anal., 276, 2901 – 2935 (2019). Received 28.08.19, after revision — 27.04.21 ISSN 1027-3190. Укр. мат. журн., 2021, т. 73, № 11
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spelling umjimathkievua-article-10502025-03-31T08:46:33Z Generalized Picone identity for Finsler $p$-Laplacian and its applications Generalized Picone identity for Finsler $p$-Laplacian and its applications Dwivedi, G. Dwivedi, G. Picone identity Finsler p-Laplacian Picone identity Finsler p-Laplacian UDC 517.9 We prove a generalized Picone-type identity for Finsler $p$-Laplacian and use it to establish some qualitative results for some boundary-value problems involving Finsler $p$-Laplacian. &amp;nbsp; УДК 517.9 Узагальнена тотожнiсть Пiконе для $p$ -лапласiана Фiнслера та її застосування Доведено узагальнену тотожність типу Піконе для $p$-лапласіана Фінслера, яку потім використано для отримання деяких якісних результатів для граничних задач, що включають $p$-лапласіан Фінслера. Institute of Mathematics, NAS of Ukraine 2021-11-23 Article Article application/pdf https://umj.imath.kiev.ua/index.php/umj/article/view/1050 10.37863/umzh.v73i11.1050 Ukrains’kyi Matematychnyi Zhurnal; Vol. 73 No. 11 (2021); 1451 - 1460 Український математичний журнал; Том 73 № 11 (2021); 1451 - 1460 1027-3190 en https://umj.imath.kiev.ua/index.php/umj/article/view/1050/9155 Copyright (c) 2021 Gaurav Dwivedi
spellingShingle Dwivedi, G.
Dwivedi, G.
Generalized Picone identity for Finsler $p$-Laplacian and its applications
title Generalized Picone identity for Finsler $p$-Laplacian and its applications
title_alt Generalized Picone identity for Finsler $p$-Laplacian and its applications
title_full Generalized Picone identity for Finsler $p$-Laplacian and its applications
title_fullStr Generalized Picone identity for Finsler $p$-Laplacian and its applications
title_full_unstemmed Generalized Picone identity for Finsler $p$-Laplacian and its applications
title_short Generalized Picone identity for Finsler $p$-Laplacian and its applications
title_sort generalized picone identity for finsler $p$-laplacian and its applications
topic_facet Picone identity
Finsler p-Laplacian
Picone identity
Finsler p-Laplacian
url https://umj.imath.kiev.ua/index.php/umj/article/view/1050
work_keys_str_mv AT dwivedig generalizedpiconeidentityforfinslerplaplaciananditsapplications
AT dwivedig generalizedpiconeidentityforfinslerplaplaciananditsapplications