The Cubic Szeg\h{o} Equation with a Linear Perturbation

preprint2015arXivOpen access

Abstract

We consider the following Hamiltonian equation on the L2L^2 Hardy space on the circle S1S^1 , i∂_tu=Π(∣u∣2u)+α(u∣1),α∈R,i\partial\_ t u = Π(|u|^ 2 u) + α(u|1) , α\in\mathbb{R} , where ΠΠ is the Szegő projector. The above equation with α=0α= 0 was introduced by G{é}rard and Grellier as an important mathematical model [5, 7, 3]. In this paper, we continue our studies started in [22], and prove our system is completely integrable in the Liouville sense. We study the motion of the singular values of the related Hankel operators and find a necessary condition of norm explosion. As a consequence, we prove that the trajectories of the solutions will stay in a compact subset, while more initial data will lead to norm explosion in the case α>0α>0.

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