EXISTENCE AND REGULARITY FOR CRITICAL ANISOTROPIC EQUATIONS WITH CRITICAL DIRECTIONS
18 pages
English

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EXISTENCE AND REGULARITY FOR CRITICAL ANISOTROPIC EQUATIONS WITH CRITICAL DIRECTIONS

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18 pages
English
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EXISTENCE AND REGULARITY FOR CRITICAL ANISOTROPIC EQUATIONS WITH CRITICAL DIRECTIONS JEROME VETOIS Abstract. We establish existence and regularity results for doubly critical anisotropic equa- tions in domains of the Euclidean space. In particular, we answer a question posed by Fra- gala–Gazzola–Kawohl [24] when the maximum of the anisotropic configuration coincides with the critical Sobolev exponent. 1. Introduction In this paper, we investigate existence and regularity for doubly critical anisotropic equa- tions. In dimension n ≥ 2, we provide ourselves with an anisotropic configuration ??p = (p1, . . . , pn) with pi > 1 for all i = 1, . . . , n. We let D1, ??p (?) be the anisotropic Sobolev space defined as the completion of the vector space of all smooth functions with compact support in ? with respect to the norm ?u?D1,??p (?) = ∑n i=1 ?∂u/∂xi?Lpi (?). We are concerned with the following anisotropic problem of critical growth { ?∆??p u = ? |u| p??2 u in ? , u ? D1, ??p (?) , (1.1) on domains ? in the Euclidean space Rn, where ? is a positive real number, p? is the critical Sobolev exponent (see (1.3) below), and ∆??p is the anisotropic Laplace operator defined by ∆??p u = n∑ i=1 ∂ ∂xi ?pixiu , (1.2) where ?pixiu = |∂u/∂xi| pi?2 ∂u/∂xi for all i = 1, .

  • configuration ??p

  • nonnegative

  • result

  • ∂xi

  • then there

  • let n?

  • critical anisotropic

  • existence result


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EXISTENCE AND REGULARITY FOR CRITICAL ANISOTROPIC EQUATIONS WITH CRITICAL DIRECTIONS ´ ˆ ´ JEROME VETOIS
Abstract. We establish existence and regularity results for doubly critical anisotropic equa-tions in domains of the Euclidean space. In particular, we answer a question posed by Fra-gala`GazzolaKawohl[24]whenthemaximumoftheanisotropiccongurationcoincideswith the critical Sobolev exponent.
1. Introduction In this paper, we investigate existence and regularity for doubly critical anisotropic equa-tions. In dimension n 2, we provide ourselves with an anisotropic configuration −→ p = ( p 1 , . . . , p n ) with p i > 1 for all i 1 , . . . , n . We let D 1 , p ( Ω ) be the anisotropic Sobolev space = defined as the completion of the vector space of all smooth functions with compact support in Ω with respect to the norm k u k D 1 , −→ p ( Ω ) = P in =1 k ∂u/∂x i k L pi ( Ω ) . We are concerned with the following anisotropic problem of critical growth λ p 2 ( u Δ D p 1 , u p =( Ω ) | ,u | u in Ω , (1.1) on domains Ω in the Euclidean space R n , where λ is a positive real number, p is the critical Sobolev exponent (see (1.3) below), and Δ −→ p is the anisotropic Laplace operator defined by Δ −→ p u = i = n X x i r xp ii u , (1.2) 1 where r p i u = | ∂u/∂x i | p i 2 ∂u/∂x i for all i = 1 , . . . , n . As one can check, Δ −→ p involves di-x i rectional derivatives with distinct weights. Anisotropic operators appear in several places in the literature. Recent references can be found in physics [3, 7], in biology [11], and in image processing [46]. We consider in this paper the doubly critical situation p + = p , where p + = max ( p 1 , . . . , p n ) is the maximum value of the anisotropic configuration and p is the critical Sobolev exponent for the embeddings of the anisotropic Sobolev space D 1 , −→ p ( Ω ) into Lebesgue spaces. In this setting, not only the nonlinearity has critical growth, but the operator itself has critical growth in particular directions of the Euclidean space. As a remark, the notion of critical direction is a pure anisotropic notion which does not exist when dealing with the Laplace operator or the p -Laplace operator. Given i = 1 , . . . , n , the i -th direction is said to be critical if p i = p , resp. subcritical if p i < p . Critical directions induce a failure in the rescaling invariance rule associated with (1.1).
Date : July 16, 2010. Published in Advances in Differential Equations 16 (2011), no. 1/2, 61–83. 1
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