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Complex tangential characterizations of Hardy-Sobolev spaces of holomorphic functions.

Sandrine Grellier — 1993

Revista Matemática Iberoamericana

Let Ω be a C-domain in Cn. It is well known that a holomorphic function on Ω behaves twice as well in complex tangential directions (see [GS] and [Kr] for instance). It follows from well known results (see [H], [RS]) that some converse is true for any kind of regular functions when Ω satisfies (P)    The real tangent space is generated by the Lie brackets of real and imaginary parts of complex tangent vectors In this paper...

Behavior of holomorphic functions in complex tangential directions in a domain of finite type in C.

Sandrine Grellier — 1992

Publicacions Matemàtiques

Let Ω be a domain in C. It is known that a holomorphic function on Ω behaves better in complex tangential directions. When Ω is of finite type, the best possible improvement is quantified at each point by the distance to the boundary in the complex tangential directions (see the papers on the geometry of finite type domains of Catlin, Nagel-Stein and Wainger for precise definition). We show that this improvement is characteristic: for a holomorphic function, a regularity in complex tangential directions...

Hankel operators and weak factorization for Hardy-Orlicz spaces

Aline BonamiSandrine Grellier — 2010

Colloquium Mathematicae

We study the holomorphic Hardy-Orlicz spaces Φ ( Ω ) , where Ω is the unit ball or, more generally, a convex domain of finite type or a strictly pseudoconvex domain in ℂⁿ. The function Φ is in particular such that ¹ ( Ω ) Φ ( Ω ) p ( Ω ) for some p > 0. We develop maximal characterizations, atomic and molecular decompositions. We then prove weak factorization theorems involving the space BMOA(Ω). As a consequence, we characterize those Hankel operators which are bounded from Φ ( Ω ) into ¹(Ω).

The cubic Szegő equation

Patrick GérardSandrine Grellier — 2010

Annales scientifiques de l'École Normale Supérieure

We consider the following Hamiltonian equation on the L 2 Hardy space on the circle, i t u = Π ( | u | 2 u ) , where Π is the Szegő projector. This equation can be seen as a toy model for totally non dispersive evolution equations. We display a Lax pair structure for this equation. We prove that it admits an infinite sequence of conservation laws in involution, and that it can be approximated by a sequence of finite dimensional completely integrable Hamiltonian systems. We establish several instability...

Problème spectral inverse et équation de Szegö cubique

Patrick GérardSandrine Grellier

Séminaire Laurent Schwartz — EDP et applications

Dans un exposé précédent [], nous avons justifié l’introduction de l’équation de Szegö cubique comme cas modèle d’équation de type Schrödinger sans dispersion. Ce cas modèle s’est révélé être intéressant sous divers aspects []. Dans cet exposé, nous nous attacherons à montrer comment la complète intégrabilité de l’équation de Szegö cubique permet de résoudre un problème spectral inverse pour les opérateurs de Hankel.

On the growth of Sobolev norms for the cubic Szegő equation

Patrick GérardSandrine Grellier

Séminaire Laurent Schwartz — EDP et applications

We report on a recent result establishing that trajectories of the cubic Szegő equation in Sobolev spaces with high regularity are generically unbounded, and moreover that, on solutions generated by suitable bounded subsets of initial data, every polynomial bound in time fails for high Sobolev norms. The proof relies on an instability phenomenon for a new nonlinear Fourier transform describing explicitly the solutions to the initial value problem, which is inherited from the Lax pair structure enjoyed...

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