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Uniqueness in Rough Almost Complex Structures, and Differential Inequalities

Jean-Pierre Rosay (2010)

Annales de l’institut Fourier

The study of J -holomorphic maps leads to the consideration of the inequations | u z ¯ | C | u | , and | u z ¯ | ϵ | u z | . The first inequation is fairly easy to use. The second one, that is relevant to the case of rough structures, is more delicate. The case of u vector valued is strikingly different from the scalar valued case. Unique continuation and isolated zeroes are the main topics under study. One of the results is that, in almost complex structures of Hölder class 1 2 , any J -holomorphic curve that is constant on a non-empty...

Uniqueness results for the Minkowski problem extended to hedgehogs

Yves Martinez-Maure (2012)

Open Mathematics

The classical Minkowski problem has a natural extension to hedgehogs, that is to Minkowski differences of closed convex hypersurfaces. This extended Minkowski problem is much more difficult since it essentially boils down to the question of solutions of certain Monge-Ampère equations of mixed type on the unit sphere 𝕊 n of ℝn+1. In this paper, we mainly consider the uniqueness question and give first results.

Upper and Lower Solutions Method for Darboux Problem for Fractional Order Implicit Impulsive Partial Hyperbolic Differential Equations

Saïd Abbas, Mouffak Benchohra (2012)

Acta Universitatis Palackianae Olomucensis. Facultas Rerum Naturalium. Mathematica

In this paper we investigate the existence of solutions for the initial value problems (IVP for short), for a class of implicit impulsive hyperbolic differential equations by using the lower and upper solutions method combined with Schauder’s fixed point theorem.

Upper bounds for a class of energies containing a non-local term

Arkady Poliakovsky (2010)

ESAIM: Control, Optimisation and Calculus of Variations

In this paper we construct upper bounds for families of functionals of the form E ε ( φ ) : = Ω ε | φ | 2 + 1 ε W ( φ ) d x + 1 ε N | H ¯ F ( φ ) | 2 d x where Δ H ¯ u = div { χ Ω u}. Particular cases of such functionals arise in Micromagnetics. We also use our technique to construct upper bounds for functionals that appear in a variational formulation of the method of vanishing viscosity for conservation laws.

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