Partial Differential Equations
Singular quasilinear elliptic equations and Hölder regularity
[Régularité höldérienne pour des équations quasi-linéaires elliptiques singulières]
Comptes Rendus. Mathématique, Tome 350 (2012) no. 7-8, pp. 383-388.

Nous démontrons la régularité höldérienne (Théorème 2.1) des solutions faibles des équations quasi-linéaires elliptiques singulières de la forme suivante :

{Δpu=K(x)uδ+g(x)in Ω;u|Ω=0,u>0in Ω,(P)
Ω est un ouvert borné régulier, 1<p<, δ>0, KLloc(Ω) satisfait 0K(x)constdist(x,Ω)ω pour p.p. xΩ, 0<ω<1+(1δ)(11p) et 0gL(Ω). Théorème 2.1 combiné avec le théorème du point fixe de Schauder permet de démontrer lʼexistence de solutions faibles de systèmes elliptiques quasi-linéaires singuliers de la forme (PS) (voir Introduction).

We prove the Hölder regularity (Theorem 2.1) for weak solutions to singular quasilinear elliptic equations whose prototype is

{Δpu=K(x)uδ+g(x)in Ω;u|Ω=0,u>0in Ω,(P)
where Ω is an open bounded domain with smooth boundary, 1<p<, δ>0, KLloc(Ω) satisfies 0K(x)constdist(x,Ω)ω for a.e. xΩ, 0<ω<1+(1δ)(11p), and 0gL(Ω). Theorem 2.1 together with the Schauder fixed point theorem can be used to obtain the existence of weak solutions to the singular quasilinear elliptic system (PS) described in the Introduction.

Reçu le :
Accepté le :
Publié le :
DOI : 10.1016/j.crma.2012.04.007
Giacomoni, Jacques 1 ; Schindler, Ian 2 ; Takáč, Peter 3

1 Laboratoire de mathématiques et de leurs applications - UMR CNRS 5142, bâtiment IPRA, université de Pau et des Pays de lʼAdour, avenue de lʼuniversité, BP 1155, 64013 Pau, France
2 MIP-CEREMATH / bâtiment C, manufacture des tabacs, allée de Brienne 21, 31000 Toulouse, France
3 Institut für Mathematik, Universität Rostock, Ulmenstraße 69, Haus 3, 18055 Rostock, Germany
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Giacomoni, Jacques; Schindler, Ian; Takáč, Peter. Singular quasilinear elliptic equations and Hölder regularity. Comptes Rendus. Mathématique, Tome 350 (2012) no. 7-8, pp. 383-388. doi : 10.1016/j.crma.2012.04.007. http://www.numdam.org/articles/10.1016/j.crma.2012.04.007/

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