TIME DEPENDENT GINZBURG - LANDAU EQUATIONS IN SPIN GLASSES

It is not a problem for us, since in our final proof of Theorem 1.2, we only need two independent smooth solutions wrt (d, γ 1 , γ 2 ) and having bounded behaviors at 0.. , 4, for

The proof of our result is obtained by the combination of two main ideas: the coupling and the Foias-Prodi estimate. The first subsection is a simple example devoted to understand

Null controllability of the complex Ginzburg–Landau equation Contrôlabilité à zéro de l’équation de Ginzburg–Landau complexe.. Lionel Rosier a,b, ∗ , Bing-Yu

Vol. - In this paper we study the structure of certain level set of the Ginzburg-Landau functional which has similar topology with the configuration space. As an

Using physical reasoning based on Maxwell’s equations, he predicted that the interface separating the normal from the superconducting regions should evolve according to a

Annales de l’Institut Henri Poincaré - Physique theorique.. We have by a simple calculation From this and the fact that 9D is bounded we have. here we have used

Annales de l’Institut Henri Poincaré - Physique theorique - 0246-0211 Vol.. Nous ameliorons Ie resultat d’un article anterieur [7] ]. de meme titre.. SOLUTIONS TO THE

As observed above, if α ≥ 4/N, then negative energy, finite-variance solutions of the nonlinear Schr¨ odinger equation blow up in finite time.. We have the