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Decay estimates and smoothness for solutions of the dispersion managed non-linear Schrödinger equation.Commun.Math.Phys.286(2009 (0)

by D Hundertmark, Y-R Lee
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EXPONENTIAL DECAY OF DISPERSION MANAGED SOLITONS FOR VANISHING AVERAGE DISPERSION

by M. Burak Erdoğan , Dirk Hundertmark, Young-ran Lee , 2008
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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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... 1 [0,1], Kunze’s existence proof, [30], shows that the maximizer is bounded. In [48] Stanislavova then showed that Kunze’s maximizer is infinitely often differentiable. Only recently it was shown in =-=[24]-=- that any weak solution f ∈ L 2 (R) of the dispersion management equation (1.22) is a Schwartz function, i.e., it is infinitely often differentiable and all its derivatives decay faster than algebraic...

SUPER-EXPONENTIAL DECAY OF DIFFRACTION MANAGED SOLITONS

by Dirk Hundertmark, Young-ran Lee
"... Abstract. This is the second part of a series of papers where we develop rigorous decay estimates for breather solutions of an averaged version of the non-linear Schrödinger equation. In this part we study the diffraction managed discrete nonlinear Schrödinger equation, an equation which describes c ..."
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Abstract. This is the second part of a series of papers where we develop rigorous decay estimates for breather solutions of an averaged version of the non-linear Schrödinger equation. In this part we study the diffraction managed discrete nonlinear Schrödinger equation, an equation which describes coupled waveguide arrays with periodic diffraction management geometries. We show that, for vanishing average diffraction, all solutions of the non-linear and non-local diffraction management equation decay super-exponentially. As a byproduct of our method, we also have a simple proof of existence of diffraction managed solitons in the case of vanishing average diffraction. 1.
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...ability of solutions of (1.4) for dav = 0 and initial conditions close to a minimizer. In this paper we continue our study of regularity properties of the dispersion management technique initiated in =-=[16]-=- and study the decay properties of diffraction management solitons for vanishing average dispersion, i.e., weak solutions of (1.11). Our main result is a significant strengthening of the super-polynom...

Nonlinear PDEs with modulated dispersion II: Korteweg–de Vries Equation

by K. Chouk, M. Gubinelli , 2014
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Nonlinear PDEs with modulated dispersion I: Nonlinear Schrödinger equations

by K. Chouk, M. Gubinelli , 2014
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Dispersive estimates for the Schrödinger equation

by William Robert Green - , 2010
"... In this document we explore the issue of L1 → L ∞ estimates for the solution operator of the linear Schrödinger equation, iut −∆u+ V u = 0 u(x, 0) = f(x) ∈ S(Rn). We focus particularly on the five and seven dimensional cases. We prove that the solution operator pre-composed with projection onto t ..."
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In this document we explore the issue of L1 → L ∞ estimates for the solution operator of the linear Schrödinger equation, iut −∆u+ V u = 0 u(x, 0) = f(x) ∈ S(Rn). We focus particularly on the five and seven dimensional cases. We prove that the solution operator pre-composed with projection onto the absolutely continuous spectrum of H = − ∆ + V satisfies the following estimate ‖eitHPac(H)‖L1→L ∞. |t|−n2 under certain conditions on the potential V. Specifically, in Chapter 1 we prove the dispersive estimate is satisfied with optimal assumptions on smoothness, that is V ∈ C n−32 (Rn) for n = 5, 7 assuming that zero is regular, |V (x) |. 〈x〉−β and |∇jV (x) |. 〈x〉−α, 1 ≤ j ≤ n−32 for some β> 3n+52 and α> 3, 8 in dimensions five and seven respectively. In Chapter 2 we show that for the five dimensional result one only needs that |V (x) |. 〈x〉−4 − in addition to the assumptions on the derivative and regularity of the potential. This more than cuts in half the required decay rate in the first chapter. Finally in Chapter 3 we consider a problem involving the non-linear Schrödinger equation. In particular, we consider the following equation that arises in fiber optic communication systems,

On the continuous resonant equation for NLS: I. Deterministic analysis. Preprint: arXiv:1501.03760

by Pierre Germain, Zaher Hani, Laurent Thomann, Pierre Germain, Zaher Hani, Laurent Thomann, On Nls, Hal Id Hal, Pierre Germain, Zaher Hani, Laurent Thomann
"... HAL is a multi-disciplinary open access archive for the deposit and dissemination of sci-entific research documents, whether they are pub-lished or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers. L’archive ouverte p ..."
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HAL is a multi-disciplinary open access archive for the deposit and dissemination of sci-entific research documents, whether they are pub-lished or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers. L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et a ̀ la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d’enseignement et de recherche français ou étrangers, des laboratoires publics ou privés.
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...e dispersion managed Schrödinger equation, which is obtained by averaging a nonlinear Schrödinger equation with varying dispersion. This latter equation has a similar structure as (CR). We refer to =-=[25, 11]-=- and references therein for more details. In [10] we undertake the study of (CR) with random initial conditions. We exhibit global rough dynamics (for initial data less regular than L2), and we constr...

Well-posedness and averaging of NLS with time-periodic dispersion management

by Paolo Antonelli, Jean-claude Saut, Christof Sparber - Adv. Diff. Eq , 2013
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...he form 1εγ ( t ε ) , which, as ε → 0+, leads to an effective description by a non-local equation, originally introduced in [17]. This model has been rigorously studied by several authors, see, e.g., =-=[14, 20, 30, 31, 34]-=-. In particular, it provides a mathematical basis for the definition of dispersion managed solitons [14]. DISPERSION MANAGED NLS 3 Remark 1.2. A similar situation is analyzed in [5, 13], where the aut...

ANALYTICITY OF EXTREMISERS TO THE AIRY STRICHARTZ INEQUALITY

by Dirk Hundertmark, Shuanglin Shao
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... Strichartz inequality for Airy operator e−t∂ 3 xf , and a weighted Strichartz inequality. The argument uses some ideas similar to Erdogan, Hundertmark and Lee [13], which in turn is based in part on =-=[15]-=-. In [13], it is shown that solutions to the dispersion managed non-linear Schrödinger equation in the case of zero residual dispersion are exponentially fast decaying not only in the Fourier space b...

ANALYTICITY OF EXTREMALS TO THE AIRY STRICHARTZ INEQUALITY

by Dirk Hundertmark, Shuanglin Shao
"... Abstract. We prove that there exists an extremal function to the Airy Strichartz inequality ‖e −t∂3 xf ‖ L8 t,x (R×R) ≤ C‖f‖L2 (R), by using the linear profile decomposition. Furthermore we show that, if f is an extremal, then f is exponentially decaying in the Fourier space and so f can be extende ..."
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Abstract. We prove that there exists an extremal function to the Airy Strichartz inequality ‖e −t∂3 xf ‖ L8 t,x (R×R) ≤ C‖f‖L2 (R), by using the linear profile decomposition. Furthermore we show that, if f is an extremal, then f is exponentially decaying in the Fourier space and so f can be extended to be an entire function on the complex domain. 1.
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...crucial bootstrap argument, which is refined bilinear Strichartz inequality for Airy evolution operator e−t∂3 xf, and a weighted Strichartz inequality (5). The argument is similar to Hundertmark, Lee =-=[12]-=- and Erdogan, Hundertmark, and Lee [10]. In [12], Hundertmark, Lee showed that solutions to the dispersion managed non-linear Schrödinger equation in the case of zero residual dispersion are fast deca...

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