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In this result, we develop the techniques of cite{KS1} and cite{BW} in order to determine a class of stable perturbations for a minimal mass soliton solution of a saturated, focusing nonlinear Schrodinger equation {c} i u_t + Delta u + beta (|u|^2) u = 0 u(0,x) = u_0 (x), in $reals^3$. By projecting into a subspace of the continuous spectrum of $mathcal{H}$ as in cite{S1}, cite{KS1}, we are able to use a contraction mapping similar to that from cite{BW} in order to show that there exist solutions of the form e^{i lambda_{min} t} (R_{min} + e^{i mathcal{H} t} phi + w(x,t)), where $e^{i mathcal{H} t} phi + w(x,t)$ disperses as $t to infty$. Hence, we have long time persistance of a soliton of minimal mass despite the fact that these solutions are shown to be nonlinearly unstable in cite{CP1}.
In this note, we give an alternative proof of the theorem on soliton selection for small energy solutions of nonlinear Schrodinger equations (NLS) which we studied in Anal. PDE 8 (2015), 1289-1349 and more recently in Annals of PDE (2021) 7:16. As
In this paper, we consider the long time dynamics of radially symmetric solutions of nonlinear Schrodinger equations (NLS) having a minimal mass ground state. In particular, we show that there exist solutions with initial data near the minimal mass g
We investigate the soliton dynamics for the fractional nonlinear Schrodinger equation by a suitable modulational inequality. In the semiclassical limit, the solution concentrates along a trajectory determined by a Newtonian equation depending of the fractional diffusion parameter.
In this paper we consider a class of fully nonlinear equations which cover the equation introduced by S. Donaldson a decade ago and the equation introduced by Gursky-Streets recently. We solve the equation with uniform weak $C^2$ estimates, which hold for degenerate case.
In this paper, we investigate the one-dimensional derivative nonlinear Schrodinger equations of the form $iu_t-u_{xx}+ilambdaabs{u}^k u_x=0$ with non-zero $lambdain Real$ and any real number $kgs 5$. We establish the local well-posedness of the Cauch