Abstract
The inverse spectral transform for integrable nonlinear ordinary and partial differential equations (such as the Toda lattice, Korteweg-de Vries, sine-Gordon and nonlinear Schrödinger equations) provides explicit algorithms to generate exact solutions under periodic or quasiperiodic boundary conditions. These oscillatory wavetrains may be prescribed a priori to consist of a nonlinear superposition of N phases, ?j(x, t) = ?jx + ?jt + ?0j, j = 1, ..., N, where the wave is 2p-periodic independently in each phase. This paper exhibits the numerical implementation of the inverse spectral solution of the sine-Gordon equation. The general construction is outlined and then implemented for N = 1, 2, and 3. We compute: (1) the exact theta-function solutions, (2) the Floquet spectrum of x-periodic solutions, (3) the labelling of linearized instabilities of N-phase solutions in terms of spectral data, and (4) the linearized growth rate in each unstable mode. The associated surfaces qN(x, t) are displayed to illustrate a variety of spatial and dynamical phenomena in the oscillatory solution space of this integrable system. © 1991.
| Original language | English |
|---|---|
| Pages (from-to) | 169-231 |
| Number of pages | 63 |
| Journal | Physica D: Nonlinear Phenomena |
| Volume | 48 |
| Issue number | 1 |
| Publication status | Published - Feb 1991 |
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