research

Young diagrams and N-soliton solutions of the KP equation

Abstract

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 yβ†’βˆžy\to\infty and yβ†’βˆ’βˆžy\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+,nβˆ’)({\bf n}^+,{\bf n}^-) with nΒ±=(n1Β±,...,nNΒ±),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+,nβˆ’)({\bf n}^+,{\bf n}^-). We also show that NN-soliton solutions of the KdV equation obtained by the constraint βˆ‚u/βˆ‚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

    Similar works

    Full text

    thumbnail-image

    Available Versions

    Last time updated on 01/04/2019