Topics in geometric fully nonlinear equations

Publications of YanYan Li
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For such equations, particularly for 2nd order ones, solutions generally are non-smooth and standard approaches in order to define a "weak solution" do not apply: classical, strong almost everywhere, weak, measure-valued and distributional solutions either do not exist or may not even be defined. The main reason for the latter failure is that, the standard idea of using "integration-by-parts" in order to pass derivatives to smooth test functions by duality, is not available for non-divergence structure PDE.

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Convergence

vary according to the underline geometric situation. In this lecture notes, we will restrict ourselves on fully nonlinear elliptic and parabolic equations related to. For geometric applications, the most important class of fully nonlinear elliptic This fully nonlinear equation although elliptic does not fit directly into the fully To fix the ideas, we will sketch a proof, using spherical reflection, of Alexandrov's.

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However, a soliton is a solitary wave having the additional property that other solitons can pass through it without changing its shape. There are no general methods guaranteed to find closed form solutions to non-linear PDEs. Figure 5 shows an example where a solid sphere is pinched between rigid plates. This idea was originally proposed by the Dutch mathematician, physicist, and astronomer, Christiaan Huygens, in , and is a powerful method for studying various optical phenomena [Enc]. We start with the Euler continuity and momentum equations.

These solutions will then be posted for the benefit of the other students. Schedule: Lecture 1 Overview. The subdifferential of a convex function. The real Monge-Ampere operator - definition. Lecture 2 The real Monge-Ampere operator - construction as a Borel measure using Alexandrov's theorem.

José Espinar - Escobar type Theorem for fully nonlinear Yamabe problem with boundary

Solution of the Dirichlet problem for the homogeneous real Monge-Ampere equation using an upper envelope. Lecture 3 The Cauchy problem for the homogeneous real Monge-Ampere equation. The Legendre transform in more detail. Convex hulls and the double Legendre dual: regularity and basic properties. Lecture 4 Obstruction to the solution of the Cauchy problem for the homogeneous real Monge-Ampere equation: upper and lower bounds on the subdifferential and strict convexity of the Legendre subsolution.

Lecture 5 Obstruction to the solution of the Cauchy problem for the homogeneous real Monge-Ampere equation: completion of the proof of the main theorem.

  • On some conformally invariant fully nonlinear equations (2002);
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Subequations: definition. Lecture 6 Subequations: basic properties. Subaffine functions. Functions of type F. Comparison with viscosity solutions.

Lecture 7 Subequations: rays sets and boundary defining functions. Lecture 8 Subequations: boundary defining functions for domains with non-smooth boundary, part 1. Lecture 9 Subequations: boundary defining functions for domains with non-smooth boundary, part 2.

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Lecture 10 Solving the Dirichlet problem for domains with non-smooth boundary: the main theorem. Lecture 11 Solving the Dirichlet problem for domains with non-smooth boundary: boundary defining functions for boundary components.

Lecture 12 The spacetime Lagrangian angle. Lecture 13 The subequation associated to the spacetime Lagrangian angle. Lecture 14 The subequation associated to the spacetime Lagrangian angle via degenerate ellipticity. Lecture 15 Constructing a solution to the Dirichlet problem associated to the spacetime Lagrangian angle. Lecture 16 Subequations on Riemannian manifolds: Overview and main results. Lecture 18 Subequations on Riemannian manifolds: topological G-structures, local jet equivalence. Lecture 19 Subequations on Riemannian manifolds.

Strictly F-subharmonic functions, local vs. Lecture 20 Subequations on Riemannian manifolds: local vs. Lecture 21 Subequations on Riemannian manifolds: affine jet equivalence, the Calabi-Yau equation.