228 research outputs found

    Rogue waves of the Fokas-Lenells equation

    Full text link
    The Fokas-Lenells (FL) equation arises as a model eqution which describes for nonlinear pulse propagation in optical fibers by retaining terms up to the next leading asymptotic order (in the leading asymptotic order the nonlinear Schr\"odinger (NLS) equation results). Here we present an explicit analytical representation for the rogue waves of the FL equation. This representation is constructed by deriving an appropriate Darboux transformation (DT) and utilizing a Taylor series expansion of the associated breather solution. when certain higher-order nonlinear effects are considered, the propagation of rogue waves in optical fibers is given.Comment: 7 pages, 3 figure

    The hierarchy of higher order solutions of the derivative nonlinear Schr\"odinger equation

    Full text link
    In this paper, we provide a simple method to generate higher order position solutions and rogue wave solutions for the derivative nonlinear Schr\"odinger equation. The formulae of these higher order solutions are given in terms of determinants. The dynamics and structures of solutions generated by this method are studied

    The higher order Rogue Wave solutions of the Gerdjikov-Ivanov equation

    Full text link
    We construct higher order rogue wave solutions for the Gerdjikov-Ivanov equation explicitly in term of determinant expression. Dynamics of both soliton and non-soliton solutions is discussed. A family of solutions with distinct structures are presented, which are new to the Gerdjikov-Ivanov equation

    The Rogue Wave and breather solution of the Gerdjikov-Ivanov equation

    Full text link
    The Gerdjikov-Ivanov (GI) system of qq and rr is defined by a quadratic polynomial spectral problem with 2×22 \times 2 matrix coefficients. Each element of the matrix of n-fold Darboux transformation of this system is expressed by a ratio of (n+1)×(n+1)(n+1)\times (n+1) determinant and n×nn\times n determinant of eigenfunctions, which implies the determinant representation of q[n]q^{[n]} and r[n]r^{[n]} generated from known solution qq and rr. By choosing some special eigenvalues and eigenfunctions according to the reduction conditions q[n]=−(r[n])∗q^{[n]}=-(r^{[n]})^*, the determinant representation of q[n]q^{[n]} provides some new solutions of the GI equation. As examples, the breather solutions and rogue wave of the GI is given explicitly by two-fold DT from a periodic "seed" with a constant amplitude.Comment: 8 figures, 17 page
    • …
    corecore