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Tao: A refined global well-posedness result for Schrodinger equations with derivative, preprint arXiv:math.AP/0110026, (2001)

by J Colliander, M Keel, G Staffilani, H Takaoka, T
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SHARP GLOBAL WELL-POSEDNESS FOR KDV AND MODIFIED KDV ON R AND T

by J. Colliander, M. Keel, G. Staffilani, H. Takaoka, T. Tao
"... 1.1. GWP below the conservation law 707 1.2. The operator I and almost conserved quantities 708 ..."
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1.1. GWP below the conservation law 707 1.2. The operator I and almost conserved quantities 708
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...: s> 3 4 [21] F: s> 3 4 ,L2 small [21] F: big L 2 blows up [38] k ≥ 6 sk = 1 2 − F: s<sk, [33];D:?? s ≥ sk, [31] D: s ≥ 1, F: small H 2 k 1 F: big H 1 blows up ?? Our results here and elsewhere [16], =-=[14]-=-, [17] suggest that local well-posedness implies global well-posedness in subcritical dispersive initial value problems. In particular, we believe our methods will extend to prove GWP of mKdV in H 1 4...

EXPONENTIAL DECAY OF DISPERSION MANAGED SOLITONS FOR VANISHING AVERAGE DISPERSION

by M. Burak Erdoğan , Dirk Hundertmark, Young-ran Lee , 2008
"... ..."
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GLOBAL WELL-POSEDNESS FOR THE L 2-CRITICAL NONLINEAR SCHRÖDINGER EQUATION IN HIGHER DIMENSIONS

by Daniela De Silva, Nata ˇ Sa Pavlović, Gigliola Staffilani, Nikolaos Tzirakis , 2006
"... Abstract. The initial value problem for the L 2 critical semilinear Schrödinger equation in R n, n ≥ 3 is considered. We show that the problem is globally well posed in H s (R n) when 1> s> √ 7−1 3 for n = 3, and when 1> s> −(n−2)+ (n−2) 2 +8(n−2) for n ≥ 4. We ..."
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Abstract. The initial value problem for the L 2 critical semilinear Schrödinger equation in R n, n ≥ 3 is considered. We show that the problem is globally well posed in H s (R n) when 1&gt; s&gt; √ 7−1 3 for n = 3, and when 1&gt; s&gt; −(n−2)+ (n−2) 2 +8(n−2) for n ≥ 4. We
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...lobal well-posedness of (1.1)-(1.2) in the case 0 ≤ s < 1 is at this point only partially answered. Previous work establishes that in one dimension the problem is globally well-posed for s > 4/9 (see =-=[7]-=-, [19]) and in two dimensions for s ≥ 1/2 (see [8] [13]). In both these cases no scattering has been proved. In higher dimensions a first result on global well-posedness below the energy norm was pres...

Global rough solutions to the critical generalized KdV

by Luiz Gustavo Farah , 908
"... We prove that the initial value problem (IVP) for the critical generalized KdV equation ut +uxxx+(u 5)x = 0 on the real line is globally well-posed in H s (R) in s> 3/5 with the appropriate smallness assumption on the initial data. 1 ..."
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We prove that the initial value problem (IVP) for the critical generalized KdV equation ut +uxxx+(u 5)x = 0 on the real line is globally well-posed in H s (R) in s&gt; 3/5 with the appropriate smallness assumption on the initial data. 1
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...H s. (7) pb Here we use the approach introduced by Colliander,Keel, Staffilani, Takaoka and Tao in [6], called the I-method. We also explain why the refined approach introduced by the same authors in =-=[7]-=-, [8] and [10] can not be use to improve our global result stated in Theorem 1.1 (see Proposition 3.1 and Remarks 3.1-3.2 below). Note that when u0 ∈ H s (R) with s < 1 in (1), the energy (4) could be...

THE LOW REGULARITY GLOBAL SOLUTIONS FOR THE CRITICAL GENERALIZED KDV EQUATION

by Changxing Miao, Shuanglin Shao, Guixiang Xu , 908
"... Abstract. In this paper, we establish the global well-posedness for the critical generalized KdV equation with the low regularity data. To be precise, we show that a unique and global solution exists for initial data in the Sobolev space Hs`R ´ with s> 1. Of course, we require that the mass is st ..."
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Abstract. In this paper, we establish the global well-posedness for the critical generalized KdV equation with the low regularity data. To be precise, we show that a unique and global solution exists for initial data in the Sobolev space Hs`R ´ with s&gt; 1. Of course, we require that the mass is strictly less than 2 that of the ground state in the focusing case. This follows from “I-method”, which was introduced by Colliander, Keel, Staffilani, Takaoka and Tao, and improves the result in [20]. 1.
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...ssion on them). For the recent developments of I-method, we can refer to [4, 5, 6, 10, 12, 14, 15, 17, 18, 19, 31] on the applications in the context of nonlinear Schrödinger equation (NLS), refer to =-=[8, 9]-=- on the applications in the context of Schrödinger equation with derivative (DNLS), refer to [7, 11, 16, 33] on the applications in the context of gKdV equations. By using “Fourier truncation method”,...

Global well-posedness for Schrödinger equation with derivative in H 2

by Changxing Miao, Yifei Wu, Guixiang Xu - R), J. Diff. Eq , 2011
"... ar ..."
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... well-posed in H1(R) under the condition (1.2). In [30], Takaoka used Bourgain’s “Fourier truncation method” ([6, 7]) to obtain the global well-posedness in Hs(R) for s > 3233 , again under (1.2). In =-=[9, 10]-=-, I-team (Colliander-Keel-Staffilani-Takaoka-Tao) made use of the first, second generations of 2000 Mathematics Subject Classification. Primary 35Q55; Secondary 47J35. Key words and phrases. Bourgain ...

THE SEMICLASSICAL MODIFIED NONLINEAR SCHRÖDINGER EQUATION I: MODULATION THEORY AND SPECTRAL ANALYSIS

by Jeffery C. Difranco, Peter, D. Miller , 2007
"... Abstract. We study an integrable modification of the focusing nonlinear Schrödinger equation from the point of view of semiclassical asymptotics. In particular, (i) we establish several important consequences of the mixed-type limiting quasilinear system including the existence of maps that embed th ..."
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Abstract. We study an integrable modification of the focusing nonlinear Schrödinger equation from the point of view of semiclassical asymptotics. In particular, (i) we establish several important consequences of the mixed-type limiting quasilinear system including the existence of maps that embed the limiting forms of both the focusing and defocusing nonlinear Schrödinger equations into the framework of a single limiting system for the modified equation, (ii) we obtain bounds for the location of discrete spectrum for the associated spectral problem that are particularly suited to the semiclassical limit and that generalize known results for the spectrum of the nonselfadjoint Zakharov-Shabat spectral problem, and (iii) we present a multiparameter family of initial data for which we solve the associated spectral problem in terms of special functions for all values of the semiclassical scaling parameter. We view our results as part of a broader project to analyze the semiclassical limit of the modified nonlinear Schrödinger equation via the noncommutative steepest descent procedure of Deift and Zhou, and we also present a self-contained development of a Riemann-Hilbert problem of inverse scattering that differs from those given in the literature and that is well-adapted to semiclassical asymptotics. 1.
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...a leading to spectral singularities and hence is not inconsistent with the Hayashi-Ozawa conjecture. 50 (263)the Cauchy problem associated to the derivative NLS equation (262) (see in addition [10], =-=[11]-=-, [22], [24], [34], and [35]) all differing in detail but all granting existence of a unique solution under either a sufficiently small L 2 (R) norm or a finite lifetime condition. All of these result...

Ground states for the higher order dispersion managed NLS equation in the absence of average dispersion

by Markus Kunze , Jamison Moeser , Vadim Zharnitsky - J. Differential Equations
"... Abstract The problem of existence of ground states in higher order dispersion managed NLS equation is considered. The ground states are stationary solutions to dispersive equations with nonlocal nonlinearity which arise as averaging approximations in the context of strong dispersion management in o ..."
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Abstract The problem of existence of ground states in higher order dispersion managed NLS equation is considered. The ground states are stationary solutions to dispersive equations with nonlocal nonlinearity which arise as averaging approximations in the context of strong dispersion management in optical communications. The main result of this note states that the averaged equation possesses ground state solutions in the practically and conceptually important case of the vanishing residual dispersions.

On non-local variational problems with lack of compactness related to non-linear optics

by Dirk Hundertmark, Young-ran Lee , 2010
"... Abstract. We give a simple proof of existence of solutions of the dispersion management and diffraction management equations for zero average dispersion, respectively diffraction. These solutions are found as maximizers of non-linear and non-local variational problems which are invariant under a lar ..."
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Abstract. We give a simple proof of existence of solutions of the dispersion management and diffraction management equations for zero average dispersion, respectively diffraction. These solutions are found as maximizers of non-linear and non-local variational problems which are invariant under a large non-compact group. Our proof of existence of maximizer is rather direct and avoids the use of Lions ’ concentration compactness argument or Ekeland’s variational principle. 1.
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...sitive on a set of positive Lebesgue measure.22 D. HUNDERTMARK AND Y.-R. LEE The proof of the multi-linear estimates is based on the by now well-known bilinear Strichartz estimate, see, for example, =-=[6, 13, 28, 43]-=-, ‖Ttf1Ttf2‖ L 2 (R×R,dtdx) � 1 √ dist(supp f1, supp f2) ‖f1‖ L 2 (R)‖f2‖ L 2 (R). (B.9) going back to [6]. For a simple explicit proof of (B.9), see for example, [31] or [24]. Now assume that the...

MASS CONCENTRATION PHENOMENON FOR THE QUINTIC NONLINEAR SCHRÖDINGER EQUATION IN 1D

by Nikolaos Tzirakis , 2006
"... Abstract. We consider the L 2-critical quintic focusing nonlinear Schrödinger equation (NLS) on R. It is well known that H 1 solutions of the aforementioned equation blow-up in finite time. In higher dimensions, for H 1 spherically symmetric blow-up solutions of the L 2-critical focusing NLS, there ..."
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Abstract. We consider the L 2-critical quintic focusing nonlinear Schrödinger equation (NLS) on R. It is well known that H 1 solutions of the aforementioned equation blow-up in finite time. In higher dimensions, for H 1 spherically symmetric blow-up solutions of the L 2-critical focusing NLS, there is a minimal amount of concentration of the L 2-norm (the mass of the ground state) at the origin. In this paper we prove the existence of a similar phenomenon for the 1d case and rougher initial data, (u0 ∈ H s, s &lt; 1), without any additional assumption. 1.
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...nstant in the Gagliardo-Nirenberg inequality 1 6 ‖u‖6 L 6 ≤ C 2 ‖∇u‖2 L 2‖u‖ 4 L 2. We used the “I-method” that was recently introduced by J. Colliander, M. Keel, G. Stafillani, H.Takaoka, and T.Tao, =-=[5, 7, 8, 9]-=-. This method allows us to define a modification of the energy functional, that is “almost conserved” that is, its time derivative decays with respect to a very large parameter. Since an implementatio...

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