International audienceWe consider a nonlinear Schrödinger equation with double power nonlinearity, where one power is focusing and mass critical and the other mass sub-critical. Classical variational arguments ensure that initial data with mass less than the mass of the ground state of the mass critical problem lead to global in time solutions. We are interested by the threshold dynamic and in particular by the existence of finite time blow up minimal solutions. For the mass critical problem, such an object exists thanks to the explicit conformal symmetry, and is in fact unique. For the focusing double power nonlinearity, we exhibit a new class of minimal blow up solutions with blow up rates deeply affected by the double power nonlinearity....
We establish the classification of minimal mass blow-up solutions of the L2 critical inhomogeneous n...
We establish the classification of minimal mass blow-up solutions of the L2 critical inhomogeneous n...
AbstractWe consider the solution of the nonlinear Schrödinger equation i ∂u∂t = −Δu + f(u) and u(0, ...
International audienceWe consider a nonlinear Schrödinger equation with double power nonlinearity, w...
International audienceWe consider a nonlinear Schrödinger equation with double power nonlinearity, w...
International audienceWe consider a nonlinear Schrödinger equation with double power nonlinearity, w...
International audienceWe consider a nonlinear Schrödinger equation with double power nonlinearity, w...
We consider the following nonlinear Schr\"{o}dinger equation with double power nonlinearities and an...
AbstractIn this paper we consider the blow up phenomenon of critical nonlinear Schrödinger equations...
Abstract. We consider a nonlinear Schrödinger equation with double power nonlinearity i∂tu+∆u+ |u| ...
AbstractIn this paper, we mainly discuss the radial case for L2 critical nonlinear Schrödinger equat...
We consider the critical nonlinear Schrödinger equation iut = −∆u − |u | 4N u with initial condition...
International audienceIn this paper, we consider the nonlinear Schrödinger equation with the super c...
In this paper, we consider the nonlinear Schrödinger equation with the super critical power of nonli...
AbstractWe consider the energy supercritical defocusing nonlinear Schrödinger equation $$\begin{alig...
We establish the classification of minimal mass blow-up solutions of the L2 critical inhomogeneous n...
We establish the classification of minimal mass blow-up solutions of the L2 critical inhomogeneous n...
AbstractWe consider the solution of the nonlinear Schrödinger equation i ∂u∂t = −Δu + f(u) and u(0, ...
International audienceWe consider a nonlinear Schrödinger equation with double power nonlinearity, w...
International audienceWe consider a nonlinear Schrödinger equation with double power nonlinearity, w...
International audienceWe consider a nonlinear Schrödinger equation with double power nonlinearity, w...
International audienceWe consider a nonlinear Schrödinger equation with double power nonlinearity, w...
We consider the following nonlinear Schr\"{o}dinger equation with double power nonlinearities and an...
AbstractIn this paper we consider the blow up phenomenon of critical nonlinear Schrödinger equations...
Abstract. We consider a nonlinear Schrödinger equation with double power nonlinearity i∂tu+∆u+ |u| ...
AbstractIn this paper, we mainly discuss the radial case for L2 critical nonlinear Schrödinger equat...
We consider the critical nonlinear Schrödinger equation iut = −∆u − |u | 4N u with initial condition...
International audienceIn this paper, we consider the nonlinear Schrödinger equation with the super c...
In this paper, we consider the nonlinear Schrödinger equation with the super critical power of nonli...
AbstractWe consider the energy supercritical defocusing nonlinear Schrödinger equation $$\begin{alig...
We establish the classification of minimal mass blow-up solutions of the L2 critical inhomogeneous n...
We establish the classification of minimal mass blow-up solutions of the L2 critical inhomogeneous n...
AbstractWe consider the solution of the nonlinear Schrödinger equation i ∂u∂t = −Δu + f(u) and u(0, ...