Dissertations / Theses on the topic 'Focusing Nonlinear schroedinger equation'

The present thesis is devoted to the investigation of certain aspects of the large time behavior of the solutions of two nonlinear Schrödinger equations in dimension three in some suitable perturbative regimes. The first model consist in a Schrödinger equation with a concentrated nonlinearity obtained considering a {point} (or contact) interaction with strength $alpha$, which consists of a singular perturbation of the Laplacian described by a self adjoint operator $H_{alpha}$, and letting the strength $alpha$ depend on the wave function: $ifrac{du}{dt}= H_alpha u$, $alpha=alpha(u)$.It is well-known that the elements of the domain of a point interaction in three dimensions can be written as the sum of a regular function and a function that exhibits a singularity proportional to $|x - x_0|^{-1}$, where $x_0$is the location of the point interaction. If $q$ is the so-called charge of the domain element $u$, i.e. the coefficient of itssingular part, then, in order to introduce a nonlinearity, we let the strength $alpha$ depend on $u$ according to the law $alpha=-nu|q|^sigma$, with $nu > 0$. This characterizes the model as a focusing NLS with concentrated nonlinearity of power type. In particular, we study orbital and asymptotic stability of standing waves for such a model. We prove the existence of standing waves of the form $u (t)=e^{iomega t}Phi_{omega}$, which are orbitally stable in the range $sigma in (0,1)$, and orbitally unstable for $sigma geq 1.$ Moreover, we show that for $sigma in(0,frac{1}{sqrt 2}) cup left(frac{1}{sqrt{2}}, frac{sqrt{3} +1}{2sqrt{2}} right)$ every standing wave is asymptotically stable, in the following sense. Choosing an initial data close to the stationary state in the energy norm, and belonging to a natural weighted $L^p$ space which allows dispersive stimates, the following resolution holds: $u(t) =e^{iomega_{infty} t +il(t)} Phi_{omega_{infty}}+U_t*psi_{infty} +r_{infty}$, where $U_t$ is the free Schrödinger propagator,$omega_{infty} > 0$ and $psi_{infty}$, $r_{infty} inL^2(R^3)$ with $| r_{infty} |_{L^2} = O(t^{-p}) quadtextrm{as} ;; t right arrow +infty$, $p = frac{5}{4}$,$frac{1}{4}$ depending on $sigma in (0, 1/sqrt{2})$, $sigma in (1/sqrt{2}, 1)$, respectively, and finally $l(t)$ is a logarithmic increasing function that appears when $sigma in (frac{1}{sqrt{2}},sigma^*)$, for a certain $sigma^* in left(frac{1}{sqrt{2}}, frac{sqrt{3} +1}{2sqrt{2}} right]$. Notice that in the present model the admitted nonlinearities for which asymptotic stability of solitons is proved, are subcritical in the sense that it does not give rise to blow up, regardless of the chosen initial data. The second model is the energy critical focusing nonlinear Schrödinger equation $i frac{du}{dt}=-Delta u-|u|^4 u$. In this case we prove, for any $nu$ and $alpha_0$ sufficiently small, the existence of radial finite energy solutions of the form$u(t,x)=e^{ialpha(t)}lambda^{1/2}(t)W(lambda(t)x)+e^{iDeltat}zeta^*+o_{dot H^1} (1)$ as $tright arrow +infty$, where$alpha(t)=alpha_0ln t$, $lambda(t)=t^{nu}$,$W(x)=(1+frac13|x|^2)^{-1/2}$ is the ground state and $zeta^*$is arbitrarily small in $dot H^1$

Thesis (Ph. D.)--University of North Carolina at Chapel Hill, 2009.
Title from electronic title page (viewed Jun. 26, 2009). "... in partial fulfillment of the requirements for the degree of Doctor of Philosophy in the Department of Mathematics." Discipline: Mathematics; Department/School: Mathematics.

Certain conservative discretizations of the Nonlinear Schroedinger (NLS) Equation can produce irregular behavior. We consider the diagonal discretization as a conservative perturbation of the integrable discretization and study the homoclinic crossings in its nonlinear spectrum. We find that irregularity sets in for the two unstable mode regime and, in this case, many and continual homoclinic crossings occur throughout the irregular time series. We undertake an analysis to determine the mechanism that causes the "chaotic" behavior to appear in this conservatively perturbed NLS equation. This analysis involves the construction of explicit formulas for the homoclinic orbit, a description of the relevant finite dimensional phase space and a Melnikov analysis for the various regimes studied.

This work consists of a study of the complex Ginzburg-Landau equation (CGL) as a perturbation of the nonlinear Schrodinger equation (NLS) in one dimension under periodic boundary conditions. Using an averaging technique which is similar to a Melnikov method for pde's, necessary conditions are derived for the persistence of NLS solutions under the CGL perturbation. For the traveling wave solutions, these conditions are derived for a general nonlinearity and written explicitly as two equations for the two continuous parameters which determine the NLS traveling wave. It is shown using a Melnikov argument that in this case these two conditions are sufficient provided they satisfy a transversality condition. As a concrete example, the equations for the parameters are solved numerically in the important case of the CGL equation with a cubic nonlinearity. For the case of the CGL equation with a general power nonlinearity, it is proved that the NLS homoclinic orbits to rotating waves are destroyed by the CGL perturbation. Special attention is dedicated to the cubic case. For this nonlinearity, the NLS equation is a completely integrable Hamiltonian system and a much larger family of its solutions can be written explicitly. The necessary conditions for the persistence of the NLS isospectral manifold are written explicitly as a system of equations for the simple periodic eigenvalues. As an example, the conditions for an even genus two solution are written down as a system of three equations with three unknowns.

We give a proof of the long-time asymptotic behavior of the focusing nonlinear Schrödinger equation for generic initial condition in which we have simple discrete spectral data and an absence of spectral singularities. The proof relies upon the theory of Riemann-Hilbert problems and the ∂ ̄ method for nonlinear steepest descent. To leading order, the solution will appear as a multi-soliton solution as t → ∞.

The small dispersion limit of the focusing nonlinear Schroödinger equation (fNLS) exhibits a rich structure with rapid oscillations at microscopic scales. Due to the non self-adjoint scattering problem associated to fNLS, very few rigorous results exist in the semiclassical limit. The asymptotics for reectionless WKB-like initial data was worked out in [KMM03] and for the family q(x, 0) = sech^(1+(i/∈)μ in [TVZ04]. In both studies the authors observed sharp breaking curves in the space-time separating regions with disparate asymptotic behaviors. In this paper we consider another exactly solvable family of initial data, specifically the family of centered square pulses, q(x; 0) = qx[-L,L] for real amplitudes q. Using Riemann- Hilbert techniques we obtain rigorous pointwise asymptotics for the semiclassical limit of fNLS globally in space and up to an O(1) maximal time. In particular, we find breaking curves emerging in accord with the previous studies. Finally, we show that the discontinuities in our initial data regularize by the immediate generation of genus one oscillations emitted into the support of the initial data. This is the first case in which the genus structure of the semiclassical asymptotics for fNLS have been calculated for non-analytic initial data.

The present thesis is devoted to the investigation of certain aspects of the large time behavior of the solutions of two nonlinear Schrödinger equations in dimension three in some suitable perturbative regimes. The rst model consist in a Schrödinger equation with a concentrated nonlinearity obtained considering a point (or contact) interaction with strength , which consists of a singular perturbation of the Laplacian described by a selfadjoint operator H , and letting the strength depend on the wave function: i du dt = H u, = (u). It is well-known that the elements of the domain of a point interaction in three dimensions can be written as the sum of a regular function and a function that exhibits a singularity proportional to jx x0j1, where x0 is the location of the point interaction. If q is the so-called charge of the domain element u, i.e. the coe cient of its singular part, then, in order to introduce a nonlinearity, we let the strength depend on u according to the law = jqj , with > 0. This characterizes the model as a focusing NLS with concentrated nonlinearity of power type. In particular, we study orbital and asymptotic stability of standing waves for such a model. We prove the existence of standing waves of the form u(t) = ei!t !, which are orbitally stable in the range 2 (0; 1), and orbitally unstable for 1: Moreover, we show that for 2 (0; p1 2 ) [ p1 2 ; p 3+1 2 p 2 every standing wave is asymptotically stable, in the following sense. Choosing an initial data close to the stationary state in the energy norm, and belonging to a natural weighted Lp space which allows dispersive estimates, the following resolution holds: u(t) = ei!1t+il(t) !1 + Ut 1 + r1, where Ut is the free Schrödinger propagator, !1 > 0 and 1, r1 2 L2(R3) with kr1kL2 = O(tp) as t ! +1, p = 5 4 , 1 4 depending on 2 (0; 1= p 2), 2 (1= p 2; 1), respectively, and nally l(t) is a logarithmic increasing function that appears when 2 (p1 2 ; ), for a certain 2 p1 2 ; p 3+1 2 p 2 i . Notice that in the present model the admitted nonlinearities for which asymptotic stability of solitons is proved, are subcritical in the sense that it does not give rise to blow up, regardless of the chosen initial data. The second model is the energy critical focusing nonlinear Schrödinger equation i du dt = u juj4u. In this case we prove, for any and 0 su ciently small, the existence of radial nite energy solutions of the form u(t; x) = ei (t) 1=2(t)W( (t)x) + ei t + o _H1(1) as t ! +1, where (t) = 0 ln t, (t) = t , W(x) = (1+ 1 3 jxj2)1=2 is the ground state and is arbitrarily small in _H 1.

Dans le cadre des études sur l'endommagement laser liées au projet Mégajoule, nous analysons le couplage entre l'auto-focalisation induite par effet Kerr et la rétrodiffusion Brillouin stimulée pour des impulsions de durée nanoseconde se propageant dans des échantillons de silice. L'influence de la puissance d'entrée, des modulations de phase ou d'amplitude ainsi que la forme spatiale du faisceau sur la dynamique de filamentation est discutée. Nous montrons qu'une modulation d'amplitude appropriée divisant l'impulsion incidente en train d'impulsions de l'ordre de la dizaine de picosecondes supprime l'effet Brillouin pour toute puissance incidente mais réduit notablement la puissance laser disponible. A l'inverse, des impulsions modulées en phase avec une largeur spectrale comparable peuvent subir de la filamentation multiple et une auto-focalisation à distance plus courte causées par des instabilités modulationnelles. Nous démontrons cependant l'existence d'une largeur spectrale critique à partir de laquelle la rétrodiffusion peut être radicalement inhibée par une modulation de phase, même pour des fortes puissances. Cette observation reste valide pour des faisceaux de forme carrée avec des profils spatiaux plus larges, qui s'auto-focalisent beaucoup plus rapidement et se brisent en filaments multiples sur de courtes distances. L'inclusion de la génération de plasma pour limiter la croissance des ondes pompe et Stokes est finalement abordée.

Dans cette thèse, nous étudions l’influence d’un plasma non-stationnaire produit par des impulsions laser en régime d’auto-focalisation. Cette auto-focalisation est couplée à des non-linéarités Brillouin pour des impulsions nanosecondes dans les verres de silice. Elle excite différents canaux d’ionisation dans les cristaux de KDP irradiées par des impulsions femtosecondes. Tout d’abord, nous dérivons les équations de propagation des ondes optiques laser et Stokes sujettes à la filamentation due à l’effet Kerr, la rétrodiffusion Brillouin et à la génération de plasma. Dans une deuxième partie, nous présentons des résultats numériques sur la propagation non-linéaire de faisceaux LIL. Ceux-ci révèlent l’importance de la distribution temporelle de l’impulsion pompe dans la compétition entre auto-compression Kerr et la rétrodiffusion Brillouin stimulée. Ces simulations préliminaires permettent de valider le système anti-Brillouin opté pour le LMJ sur la base de faisceaux millimétriques.Dans une troisième partie, nous présentons des résultats théoriques et numériques sur la filamentation d’impulsions nanosecondes opérant dans l’ultraviolet et l’infrarouge. L’influence d’un plasma inertiel sur la dynamique de couplage de deux ondes en contre-propagation est examinée. Dans une configuration à une onde, une analyse variationnelle reproduit les caractéristiques globales d’un équilibre quasi-stationnaire entre auto-compression Kerr et défocalisation plasma. Toutefois, cet équilibre cesse pour faire place à des instabilités modulationnelles induites par rétroaction du plasma sur l’onde de pompe. Nous montrons que des modulations de phase supprimant la rétrodiffusion Brillouin permettent d’inhiber ces instabilités plasma. La robustesse de ces modulations de phase est testée en présence d’un bruit aléatoire dans le profil de l’impulsion laser.Enfin, nous étudions numériquement la dynamique non-linéaire d’impulsions femtosecondes se propageant dans la silice et le KDP. Premièrement, nous montrons que la présence de défauts impliquant moins de photons pour exciter un électron de la bande de valence à la bande de conduction promeut des intensités de filamentation plus élevées. Ensuite, nous comparons la dynamique de filamentation dans la silice avec celle dans un cristal KDP. Le modèle d’ionisation pour le KDP prend en compte la présence de défauts et la dynamique électrons-trous. Nous montrons que la dynamique de propagation dans la silice et le KDP présente des analogies remarquables pour des rapports de puissance incidente sur puissance critique équivalents.La conclusion nous permet de résumer les résultats originaux obtenus dans le cadre de cette thèse et d’en discuter des développements ultérieurs possibles
In this thesis, we study the role of an inertial plasma reponse produced by laser pulses in self-focusing regime. Self-focusing is coupled with Brillouin nonlinearities for nanosecond pulses in silica glasses. For femtosecond pulses propagating in KDP crystals, self-focusing excites various ionization chanels. First of all, we derive the propagation equations for the pump and Stokes waves, subjected to filamentation due to optical Kerr effect, stimulated Brillouin scattering and plasma generation. In the second part, we present numerical results on the nonlinear propagation of LIL laser beams. These results show that temporal distribution of the pump pulse play a key role in the competition between self-focusing and stimulated Brillouin scattering. These preliminary results valide the anti-Brillouin system opted on the MegaJoule laser (LMJ) on the basis of milimetric-size laser beam.In a third part, we present numerical and theoretical results on the filamentation in fused silica of nanosecond light pulses operating in ultraviolet and infrared range. Emphasis is put on the action of a dynamical plasma reponse on two counterpropagating waves. For a single wave, we develop a variational analysis which reproduces global propagation features for a quasistationary balance between self-focusing and plasma defocusing. However, such a quasistionary balance ceases to clean up modulational instabilites induced by plasma retroaction on the pump wave. We show that phase modulations supress both simulated Brillouin scattering and plasma instabilities. The robustness of phase modulations is evaluated in presence of random fluctuations in the input pump pulse profile.Finally, we study numerically the nonlinear propagation of femtosecond pulses in fused silica and KDP. First, we show that the presence of defects involving less photons for exciting electrons from the valence band to the conduction band promotes higher filamentation intensity levels. Then, we compare the filamentation dynamic in silica and KDP crystal. The ionization model for KDP crystal takes into account the presence of defects and the electron-hole dynamics. We show that the propagation dynamics in silica and KDP are almost identical at equivalent ratios of input power over the critical power self-focusing.The summary of this thesis recalls the original results obtained and discusses the possibility of future developments

In this dissertation, we consider the equilibrium as well as near-equilibrium statistical behavior of the discretized nonlinear Schrödinger equation (NLS). We create a modified version of the Metropolis algorithm for generating empirical distributions that approximate the mixed ensemble Gibbs distribution for the NLS. The mixed ensemble is canonical in energy and microcanonical in particle number invariant. After generating and analyzing many such empirical distributions spanning a full range of equilibrium behaviors, we study their near-equilibrium responses to perturbations via linear response theory. This leads us to the discovery of a regime in which near-equilibrium ensembles resist relaxation toward equilibrium when evolved under the NLS dynamics. Within this regime, perturbed mean observables relax in two stages; they undergo a rapid disruption followed by an extremely slow equilibration. In some cases of the latter stage, there is no observable rate of decay towards equilibrium. We propose that quasiperiodicity of individual solutions may be the dynamical mechanism that underlies this two stage behavior. We exhibit a direct correspondence between the two stage regime and the regime within which quasiperiodicity prevails.

abstract: Nonlinear dispersive equations model nonlinear waves in a wide range of physical and mathematics contexts. They reinforce or dissipate effects of linear dispersion and nonlinear interactions, and thus, may be of a focusing or defocusing nature. The nonlinear Schrödinger equation or NLS is an example of such equations. It appears as a model in hydrodynamics, nonlinear optics, quantum condensates, heat pulses in solids and various other nonlinear instability phenomena. In mathematics, one of the interests is to look at the wave interaction: waves propagation with different speeds and/or different directions produces either small perturbations comparable with linear behavior, or creates solitary waves, or even leads to singular solutions. This dissertation studies the global behavior of finite energy solutions to the $d$-dimensional focusing NLS equation, $i partial _t u+Delta u+ |u|^{p-1}u=0, $ with initial data $u_0in H^1,; x in Rn$; the nonlinearity power $p$ and the dimension $d$ are chosen so that the scaling index $s=frac{d}{2}-frac{2}{p-1}$ is between 0 and 1, thus, the NLS is mass-supercritical $(s>0)$ and energy-subcritical $(s<1).$ For solutions with $ME[u_0]<1$ ($ME[u_0]$ stands for an invariant and conserved quantity in terms of the mass and energy of $u_0$), a sharp threshold for scattering and blowup is given. Namely, if the renormalized gradient $g_u$ of a solution $u$ to NLS is initially less than 1, i.e., $g_u(0)<1,$ then the solution exists globally in time and scatters in $H^1$ (approaches some linear Schr"odinger evolution as $ttopminfty$); if the renormalized gradient $g_u(0)>1,$ then the solution exhibits a blowup behavior, that is, either a finite time blowup occurs, or there is a divergence of $H^1$ norm in infinite time. This work generalizes the results for the 3d cubic NLS obtained in a series of papers by Holmer-Roudenko and Duyckaerts-Holmer-Roudenko with the key ingredients, the concentration compactness and localized variance, developed in the context of the energy-critical NLS and Nonlinear Wave equations by Kenig and Merle. One of the difficulties is fractional powers of nonlinearities which are overcome by considering Besov-Strichartz estimates and various fractional differentiation rules.
Dissertation/Thesis
Ph.D. Mathematics 2011

The historical role of nonlinear waves in developing the science of complexity, and also their physical feature of being a widespread paradigm in optics, establishes a bridge between two diverse and fundamental fields that can open an immeasurable number of new routes. In what follows, we present our most important results on nonlinear waves in classical and quantum nonlinear optics. About classical phenomenology, we lay the groundwork for establishing one uniform theory of dispersive shock waves, and for controlling complex nonlinear regimes through simple integer topological invariants. The second quantized field theory of optical propagation in nonlinear dispersive media allows us to perform numerical simulations of quantum solitons and the quantum nonlinear box problem. The complexity of light propagation in nonlinear media is here examined from all the main points of view: extreme phenomena, recurrence, control, modulation instability, and so forth. Such an analysis has a major, significant goal: answering the question can nonlinear waves do computation? For this purpose, our study towards the realization of an all-optical computer, able to do computation by implementing machine learning algorithms, is illustrated. The first all-optical realization of the Ising machine and the theoretical foundations of the random optical machine are here reported. We believe that this treatise is a fundamental study for the application of nonlinear waves to new computational techniques, disclosing new procedures to the control of extreme waves, and to the design of new quantum sources and non-classical state generators for future quantum technologies, also giving incredible insights about all-optical reservoir computing. Can nonlinear waves do computation? Our random optical machine draws the route for a positive answer to this question, substituting the randomness either with the uncertainty of quantum noise effects on light propagation or with the arbitrariness of classical, extremely nonlinear regimes, as similarly done by random projection methods and extreme learning machines.