1,259 research outputs found

    On the equivalence of different approaches for generating multisoliton solutions of the KPII equation

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    The unexpectedly rich structure of the multisoliton solutions of the KPII equation has been explored by using different approaches, running from dressing method to twisting transformations and to the tau-function formulation. All these approaches proved to be useful in order to display different properties of these solutions and their related Jost solutions. The aim of this paper is to establish the explicit formulae relating all these approaches. In addition some hidden invariance properties of these multisoliton solutions are discussed

    Soliton solutions of the Kadomtsev-Petviashvili II equation

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    We study a general class of line-soliton solutions of the Kadomtsev-Petviashvili II (KPII) equation by investigating the Wronskian form of its tau-function. We show that, in addition to previously known line-soliton solutions, this class also contains a large variety of new multi-soliton solutions, many of which exhibit nontrivial spatial interaction patterns. We also show that, in general, such solutions consist of unequal numbers of incoming and outgoing line solitons. From the asymptotic analysis of the tau-function, we explicitly characterize the incoming and outgoing line-solitons of this class of solutions. We illustrate these results by discussing several examples.Comment: 28 pages, 4 figure

    Young diagrams and N-soliton solutions of the KP equation

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    We consider NN-soliton solutions of the KP equation, (-4u_t+u_{xxx}+6uu_x)_x+3u_{yy}=0 . An NN-soliton solution is a solution u(x,y,t)u(x,y,t) which has the same set of NN line soliton solutions in both asymptotics y→∞y\to\infty and y→−∞y\to -\infty. The NN-soliton solutions include all possible resonant interactions among those line solitons. We then classify those NN-soliton solutions by defining a pair of NN-numbers (n+,n−)({\bf n}^+,{\bf n}^-) with n±=(n1±,...,nN±),nj±∈{1,...,2N}{\bf n}^{\pm}=(n_1^{\pm},...,n_N^{\pm}), n_j^{\pm}\in\{1,...,2N\}, which labels NN line solitons in the solution. The classification is related to the Schubert decomposition of the Grassmann manifolds Gr(N,2N)(N,2N), where the solution of the KP equation is defined as a torus orbit. Then the interaction pattern of NN-soliton solution can be described by the pair of Young diagrams associated with (n+,n−)({\bf n}^+,{\bf n}^-). We also show that NN-soliton solutions of the KdV equation obtained by the constraint ∂u/∂y=0\partial u/\partial y=0 cannot have resonant interaction.Comment: 22 pages, 5 figures, some minor corrections and added one section on the KdV N-soliton solution

    The dispersion-managed Ginzburg-Landau equation and its application to femtosecond lasers

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    The complex Ginzburg-Landau equation has been used extensively to describe various non-equilibrium phenomena. In the context of lasers, it models the dynamics of a pulse by averaging over the effects that take place inside the cavity. Ti:sapphire femtosecond lasers, however, produce pulses that undergo significant changes in different parts of the cavity during each round-trip. The dynamics of such pulses is therefore not adequately described by an average model that does not take such changes into account. The purpose of this work is severalfold. First we introduce the dispersion-managed Ginzburg-Landau equation (DMGLE) as an average model that describes the long-term dynamics of systems characterized by rapid variations of dispersion, nonlinearity and gain in a general setting, and we study the properties of the equation. We then explain how in particular the DMGLE arises for Ti:sapphire femtosecond lasers and we characterize its solutions. In particular, we show that, for moderate values of the gain/loss parameters, the solutions of the DMGLE are well approximated by those of the dispersion-managed nonlinear Schrodinger equation (DMNLSE), and the main effect of gain and loss dynamics is simply to select one among the one-parameter family of solutions of the DMNLSE.Comment: 22 pages, 4 figures, to appear in Nonlinearit

    On a family of solutions of the KP equation which also satisfy the Toda lattice hierarchy

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    We describe the interaction pattern in the xx-yy plane for a family of soliton solutions of the Kadomtsev-Petviashvili (KP) equation, (−4ut+uxxx+6uux)x+3uyy=0(-4u_{t}+u_{xxx}+6uu_x)_{x}+3u_{yy}=0. Those solutions also satisfy the finite Toda lattice hierarchy. We determine completely their asymptotic patterns for y→±∞y\to \pm\infty, and we show that all the solutions (except the one-soliton solution) are of {\it resonant} type, consisting of arbitrary numbers of line solitons in both aymptotics; that is, arbitrary N−N_- incoming solitons for y→−∞y\to -\infty interact to form arbitrary N+N_+ outgoing solitons for y→∞y\to\infty. We also discuss the interaction process of those solitons, and show that the resonant interaction creates a {\it web-like} structure having (N−−1)(N+−1)(N_--1)(N_+-1) holes.Comment: 18 pages, 16 figures, submitted to JPA; Math. Ge

    Noise-induced perturbations of dispersion-managed solitons

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    We study noise-induced perturbations of dispersion-managed solitons by developing soliton perturbation theory for the dispersion-managed nonlinear Schroedinger (DMNLS) equation, which governs the long-term behavior of optical fiber transmission systems and certain kinds of femtosecond lasers. We show that the eigenmodes and generalized eigenmodes of the linearized DMNLS equation around traveling-wave solutions can be generated from the invariances of the DMNLS equations, we quantify the perturbation-induced parameter changes of the solution in terms of the eigenmodes and the adjoint eigenmodes, and we obtain evolution equations for the solution parameters. We then apply these results to guide importance-sampled Monte-Carlo simulations and reconstruct the probability density functions of the solution parameters under the effect of noise.Comment: 12 pages, 6 figure

    Deconstruction of the Corso Grosseto viaduct and setup of a testing site for full scale load tests

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    BRIDGE|50 is a research project recently launched in Italy in the context of the Torino-Ceres construction works jointly with Politecnico di Milano, Politecnico di Torino, public authorities and private companies. The aim of the BRIDGE|50 research project is to investigate the residual structural performance of the Corso Grosseto 50-year-old prestressed concrete bridge through an experimental campaign. The dismantling and demolition procedures of Corso Grosseto viaduct are presented in this paper, including the setup of the field laboratory where several deck beams and pier caps will be tested up to collapse

    Building extended resolvent of heat operator via twisting transformations

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    Twisting transformations for the heat operator are introduced. They are used, at the same time, to superimpose a` la Darboux N solitons to a generic smooth, decaying at infinity, potential and to generate the corresponding Jost solutions. These twisting operators are also used to study the existence of the related extended resolvent. Existence and uniqueness of the extended resolvent in the case of NN solitons with N "ingoing" rays and one "outgoing" ray is studied in details.Comment: 15 pages, 2 figure

    Initial-boundary value problems for discrete evolution equations: discrete linear Schrodinger and integrable discrete nonlinear Schrodinger equations

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    We present a method to solve initial-boundary value problems for linear and integrable nonlinear differential-difference evolution equations. The method is the discrete version of the one developed by A. S. Fokas to solve initial-boundary value problems for linear and integrable nonlinear partial differential equations via an extension of the inverse scattering transform. The method takes advantage of the Lax pair formulation for both linear and nonlinear equations, and is based on the simultaneous spectral analysis of both parts of the Lax pair. A key role is also played by the global algebraic relation that couples all known and unknown boundary values. Even though additional technical complications arise in discrete problems compared to continuum ones, we show that a similar approach can also solve initial-boundary value problems for linear and integrable nonlinear differential-difference equations. We demonstrate the method by solving initial-boundary value problems for the discrete analogue of both the linear and the nonlinear Schrodinger equations, comparing the solution to those of the corresponding continuum problems. In the linear case we also explicitly discuss Robin-type boundary conditions not solvable by Fourier series. In the nonlinear case we also identify the linearizable boundary conditions, we discuss the elimination of the unknown boundary datum, we obtain explicitly the linear and continuum limit of the solution, and we write down the soliton solutions.Comment: 41 pages, 3 figures, to appear in Inverse Problem
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