Blow up for the critical generalized Korteweg-de Vries equation. I: Dynamics near the soliton

• 成果类型: Article
• 署名作者: Martel, Yvan; Merle, Frank; Raphael, Pierre
• 署名单位: Universite Paris Saclay; Institut Universitaire de France; Centre National de la Recherche Scientifique (CNRS); CNRS - National Institute for Mathematical Sciences (INSMI); CY Cergy Paris Universite; Centre National de la Recherche Scientifique (CNRS); CNRS - National Institute for Mathematical Sciences (INSMI); Universite Paris Saclay; Universite de Toulouse; Universite Toulouse III - Paul Sabatier; Centre National de la Recherche Scientifique (CNRS); CNRS - National Institute for Mathematical Sciences (INSMI); Institut Universitaire de France
• 刊物名称: ACTA MATHEMATICA
• ISSN/ISSBN: 0001-5962
• DOI: 10.1007/s11511-014-0109-2
• 发表日期: 2014
• 页码: 59-140
• 关键词: nonlinear schrodinger-equation; threshold solutions; global dynamics; well-posedness; ground-state; STABILITY; gkdv; mass; SINGULARITIES; CONSTRUCTION

摘要

We consider the quintic generalized Korteweg-de Vries equation (gKdV) which is a canonical mass critical problem, for initial data in H (1) close to the soliton. In earlier works on this problem, finite- or infinite-time blow up was proved for non-positive energy solutions, and the solitary wave was shown to be the universal blow-up profile, see [16], [26] and [20]. For well-localized initial data, finite-time blow up with an upper bound on blow-up rate was obtained in [18]. In this paper, we fully revisit the analysis close to the soliton for gKdV in light of the recent progress on the study of critical dispersive blow-up problems (see [31], [39], [32] and [33], for example). For a class of initial data close to the soliton, we prove that three scenarios only can occur: (i) the solution leaves any small neighborhood of the modulated family of solitons in the scale invariant L (2) norm; (ii) the solution is global and converges to a soliton as t -> a; (iii) the solution blows up in finite time T with speed Moreover, the regimes (i) and (iii) are stable. We also show that non-positive energy yields blow up in finite time, and obtain the characterization of the solitary wave at the zero-energy level as was done for the mass critical non-linear Schrodinger equation in [31].