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Blow up dynamic and upper bound on the blow up rate for critical nonlinear Schrödinger equation

Frank MerlePierre Raphael — 2002

Journées équations aux dérivées partielles

We consider the critical nonlinear Schrödinger equation i u t = - Δ u - | u | 4 N u with initial condition u ( 0 , x ) = u 0 in dimension N . For u 0 H 1 , local existence in time of solutions on an interval [ 0 , T ) is known, and there exists finite time blow up solutions, that is u 0 such that lim t T < + | u x ( t ) | L 2 = + . This is the smallest power in the nonlinearity for which blow up occurs, and is critical in this sense. The question we address is to understand the blow up dynamic. Even though there exists an explicit example of blow up solution and a class of initial data...

Dégénérescence du comportement linéaire pour l’équation des ondes semi-linéaire focalisante critique

Thomas DuyckaertsFrank Merle

Séminaire Équations aux dérivées partielles

C. Kenig et F. Merle ont montré que les solutions de l’équation des ondes focalisante quintique sur l’espace euclidien de dimension 3 ont un comportement linéaire en-dessous d’un certain seuil d’énergie. Ce comportement linéaire est caractérisé par la finitude de la norme L 8 dans les variables espace-temps. Dans cet exposé, je donnerai une estimation précise de cette norme L 8 globale pour les solutions dont l’énergie est proche de l’énergie seuil.

Isolatedness of characteristic points at blow-up for a semilinear wave equation in one space dimension

Frank MerleHatem Zaag

Séminaire Équations aux dérivées partielles

We consider the semilinear wave equation with power nonlinearity in one space dimension. We first show the existence of a blow-up solution with a characteristic point. Then, we consider an arbitrary blow-up solution u ( x , t ) , the graph x T ( x ) of its blow-up points and 𝒮 the set of all characteristic points and show that 𝒮 is locally finite. Finally, given x 0 𝒮 , we show that in selfsimilar variables, the solution decomposes into a decoupled sum of (at least two) solitons, with alternate signs and that T ( x ) forms a...

Blow up and near soliton dynamics for the L 2 critical gKdV equation

Yvan MartelFrank MerlePierre Raphaël

Séminaire Laurent Schwartz — EDP et applications

These notes present the main results of [, , ] concerning the mass critical (gKdV) equation u t + ( u x x + u 5 ) x = 0 for initial data in H 1 close to the soliton. These works revisit the blow up phenomenon close to the family of solitons in several directions: definition of the stable blow up and classification of all possible behaviors in a suitable functional setting, description of the minimal mass blow up in H 1 , construction of various exotic blow up rates in H 1 , including grow up in infinite time.

Blow up for the critical gKdV equation. II: Minimal mass dynamics

Yvan MartelFrank MerlePierre Raphaël — 2015

Journal of the European Mathematical Society

We consider the mass critical (gKdV) equation u t + ( u x x + u 5 ) x = 0 for initial data in H 1 . We first prove the existence and uniqueness in the energy space of a minimal mass blow up solution and give a sharp description of the corresponding blow up soliton-like bubble. We then show that this solution is the universal attractor of all solutions near the ground state which have a defocusing behavior. This allows us to sharpen the description of near soliton dynamics obtained in [29].

Universality of blow-up profile for small radial type II blow-up solutions of the energy-critical wave equation

Thomas DuyckaertsCarlos E. KenigFrank Merle — 2011

Journal of the European Mathematical Society

Consider the energy-critical focusing wave equation on the Euclidian space. A blow-up type II solution of this equation is a solution which has finite time of existence but stays bounded in the energy space. The aim of this work is to exhibit universal properties of such solutions. Let W be the unique radial positive stationary solution of the equation. Our main result is that in dimension 3, under an appropriate smallness assumption, any type II blow-up radial solution is essentially the sum of...

Universality of the blow-up profile for small type II blow-up solutions of the energy-critical wave equation: the nonradial case

Thomas DuyckaertsCarlos E. KenigFrank Merle — 2012

Journal of the European Mathematical Society

Following our previous paper in the radial case, we consider type II blow-up solutions to the energy-critical focusing wave equation. Let W be the unique radial positive stationary solution of the equation. Up to the symmetries of the equation, under an appropriate smallness assumption, any type II blow-up solution is asymptotically a regular solution plus a rescaled Lorentz transform of W concentrating at the origin.

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