Fourth Order Equations of Critical Sobolev Growth. Energy Function and Solutions of Bounded Energy in the Conformally Flat Case

نویسنده

  • VERONICA FELLI
چکیده

In 1983, Paneitz [23] introduced a conformally fourth order operator defined on 4-dimensional Riemannian manifolds. Branson [1] generalized the definition to n-dimensional Riemannian manifolds, n ≥ 5. Such operators have a geometrical meaning. While the conformal Laplacian is associated to the scalar curvature, the Paneitz-Branson operator is associated to a notion of Q-curvature. Possible references are Chang [2] and Chang-Yang [3]. When the manifold (M, g) is Einstein, the Paneitz-Branson operator PBg has constant coefficients. It expresses as PBg(u) = ∆ 2 gu+ ᾱ∆gu+ āu , (0.1)

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تاریخ انتشار 2008