2018
DOI: 10.1080/03605302.2018.1475489
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Global well-posedness for the derivative non-linear Schrödinger equation

Abstract: We study the Derivative Nonlinear Schrödinger (DNLS). equation for general initial conditions in weighted Sobolev spaces that can support bright solitons (but exclude spectral singularities corresponding to algebraic solitons). We show that the set of such initial data is open and dense in a weighted Sobolev space, and includes data of arbitrarily large L 2 -norm. We prove global well-posedness on this open and dense set. In a subsequent paper [10], we will use these results and a steepest descent analysis to … Show more

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Cited by 35 publications
(30 citation statements)
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“…There is also a number of works [15,16,17,29,30] where the global well-posedness of the DNLS equation was studied by means of the inverse scattering techniques. The corresponding results get rid of the smallness assumption on the mass, but require more regularity and decay on the initial data.…”
mentioning
confidence: 99%
“…There is also a number of works [15,16,17,29,30] where the global well-posedness of the DNLS equation was studied by means of the inverse scattering techniques. The corresponding results get rid of the smallness assumption on the mass, but require more regularity and decay on the initial data.…”
mentioning
confidence: 99%
“…where ρ, λ k and C k are associated to the initial data. The proof of the following theorem can be found in [22,Section 3].…”
Section: The Direct and Inverse Mapsmentioning
confidence: 99%
“…A line of results, due to Hayashi-Ozawa [8], Colliander-Keel-Staffilani-Takaoka-Tao [4], Wu [28], and Guo-Wu [7], establishes global well-posedness of the DNLS equation in H s (R) for s ≥ 1 2 , for initial data having mass less than 4π. Another line (Pelinovsky-Saalmann-Shimabukuro [23], Pelinovsky-Shimabukuro [24], and Jenkins-Liu-Perry-Sulem [12,11,10]) uses inverse scattering techniques to establish global wellposedness under stronger regularity and decay assumptions on the initial data, but without a smallness requirement on the mass.…”
Section: Introductionmentioning
confidence: 99%
“…For noninteger s, we will use a sort of 'generalized energy', comparable to u 2 Ḣs (R) , that will be defined in terms of the transmission coefficient of the DNLS spectral problem. We sketch presently the background necessary to define these objects precisely; for more details, see, for example, [1,12,11,10,13,19,24,27].…”
Section: Introductionmentioning
confidence: 99%