Affine Bernstein Problems and Monge-Ampère Equations by An-Min Li, Ruiwei Xu, Udo Simon, Fang Jia

By An-Min Li, Ruiwei Xu, Udo Simon, Fang Jia

During this monograph, the interaction among geometry and partial differential equations (PDEs) is of specific curiosity. It supplies a selfcontained advent to investigate within the final decade relating worldwide difficulties within the idea of submanifolds, resulting in a few forms of Monge-Ampère equations. From the methodical perspective, it introduces the answer of definite Monge-Ampère equations through geometric modeling suggestions. right here geometric modeling potential the right selection of a normalization and its brought about geometry on a hypersurface outlined via a neighborhood strongly convex worldwide graph. For a greater figuring out of the modeling suggestions, the authors supply a selfcontained precis of relative hypersurface idea, they derive vital PDEs (e.g. affine spheres, affine maximal surfaces, and the affine consistent suggest curvature equation). touching on modeling ideas, emphasis is on rigorously dependent proofs and exemplary comparisons among diverse modelings.

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12) in the local form Uij = Γ∗ijk Uk − Bij U with Christoffel symbols Γ∗k ij . 17. 5 Affine Gauß mappings A unimodular or Blaschke hypersurface is a triple (x, U, Y ) with (U, Y ) as equiaffine normalization of x. 3. The subsections following these statements show that the affine normalization allows to list properties similar to the Euclidean case. For a non-degenerate hypersurface we know that the mapping U : M → V ∗ always has maximal rank, thus it defines an immersion; moreover, it is easy to show that its position vector, again denoted by U , is always transversal to U (M ).

4) We will frequently need condition (c) in the apolarity condition above for explicit calculations. Equiaffine frames. From now on we shall choose an adapted frame field {x; e1 , ···, en , en+1 } such that en+1 is parallel to Y . We call such a frame an equiaffine frame; so an equiaffine frame has the three properties: (i) it is unimodular, (ii) e1 , · · ·, en are tangential, (iii) en+1 is parallel to the affine normal vector Y . This choice implies the apolarity condition and 1 Y = |H| n+2 en+1 .

It follows that en+1 = (0, · · ·, 0, 1) is the affine normal vector Y at each point of x(M ). This shows that x is a parabolic affine hypersphere. Theorem. 2) of Monge-Amp`ere type. 2 Proper affine hyperspheres Let x be an elliptic or hyperbolic affine hypersphere and assume that x locally is given as a graph of a strictly convex C ∞ -function on a domain Ω ⊂ Rn : xn+1 = f x1 , · · ·, xn , x1 , · · ·, xn ∈ Ω. 4: F : Ω → Rn where (x1 , · · ·, xn ) → (ξ1 , · · ·, ξn ) and ξi := ∂i f = ∂f ∂xi , i = 1, 2, · · ·, n.

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