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Projective Dirichlet Boundary Condition with Applications to a Geometric Problem

Projective Dirichlet Boundary Condition with Applications to a Geometric Problem
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摘要 Given a domain Ω R^n, let λ 〉 0 be an eigenvalue of the elliptic operator L := ∑i,j^n= 1δ/δxi on Ω for Dirichlet condition. For a function f ∈ L2(Ω), it is known that the linear resonance equation Lu + λu = f in Ω with Dirichlet boundary condition is not always solvable. We give a new boundary condition Pλ(u|δΩ) = g, called to be projective Dirichlet condition, such that the linear resonance equation always admits a unique solution u being orthogonal to all of the eigenfunctions corresponding to λ which satisfies ||u||2,2 ≤ C(||f||2 + ||g||2,2) under suitable regularity assumptions on δΩ and L, where C is a constant depends only on n, Ω, and L. More a priori estimates, such as W^2~'P-estimates and the C^2,α-estimates etc., are given also. This boundary condition can be viewed as a generalization of the Dirichlet condition to resonance equations and shows its advantage when applying to nonlinear resonance equations. In particular, this enables us to find the new indicatrices with vanishing mean (Cartan) torsion in Minkowski geometry. It is known that the geometry of indicatries is the foundation of Finsler geometry. Given a domain Ω R^n, let λ 〉 0 be an eigenvalue of the elliptic operator L := ∑i,j^n= 1δ/δxi on Ω for Dirichlet condition. For a function f ∈ L2(Ω), it is known that the linear resonance equation Lu + λu = f in Ω with Dirichlet boundary condition is not always solvable. We give a new boundary condition Pλ(u|δΩ) = g, called to be projective Dirichlet condition, such that the linear resonance equation always admits a unique solution u being orthogonal to all of the eigenfunctions corresponding to λ which satisfies ||u||2,2 ≤ C(||f||2 + ||g||2,2) under suitable regularity assumptions on δΩ and L, where C is a constant depends only on n, Ω, and L. More a priori estimates, such as W^2~'P-estimates and the C^2,α-estimates etc., are given also. This boundary condition can be viewed as a generalization of the Dirichlet condition to resonance equations and shows its advantage when applying to nonlinear resonance equations. In particular, this enables us to find the new indicatrices with vanishing mean (Cartan) torsion in Minkowski geometry. It is known that the geometry of indicatries is the foundation of Finsler geometry.
作者 Min JI
出处 《Acta Mathematica Sinica,English Series》 SCIE CSCD 2016年第1期11-24,共14页 数学学报(英文版)
基金 Supported by NSFC Innovation Grant(Grant No.10421101)
关键词 Elliptic resonance equation nonlinear boundary condition convex indicatrix mean tor-sion Elliptic resonance equation, nonlinear boundary condition, convex indicatrix, mean tor-sion
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参考文献8

  • 1Adams, R. A.: Sobolev Spaces, Academic Press, New York, 1975.
  • 2Bao, D., Chern, S. S., Shen, Z.: An Introduction to Riemann Finsler Geometry, Springer-Verlag, New York, 2000.
  • 3Brickell, F.: A new proof of Deicke's theorem on homogeneous functions. Proe. Amer. llgath. Soc., 16, 190 191 (1965).
  • 4Chen, Y. Z., Wu, L. C.: Elliptic Partial Differential Equations and Systems of Second Order, Academic Press, Beijing, 1991.
  • 5Deicke, A.: Uber die Finsler-Rgume mit Ai = O. Arch. Math., 4, 45-51 (1953).
  • 6Gilbarg, D., Trudinger, N. S.: Elliptic Partial Differential Equations of Second Order, Springer Verlag, Heidelberg, New York, 1997.
  • 7Ji, M., Shen, Z.: On strongly convex indicatrices in Minkowski geometry. Canad. Math. Bull., 45(2), 232-246 (2002).
  • 8Nirenberg, L.: Variational and topological methods in nonlinear problems. Bull. Amer. Math. Soc., 4, 267 302 (1986).

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