Inelastically generated solitons and anti-solitons in the perturbed KdV equation
| dc.creator | Zarmi, Yair | |
| dc.date | 2007-10-02 | |
| dc.date.accessioned | 2026-07-07T08:33:32Z | |
| dc.date.available | 2026-07-07T08:33:32Z | |
| dc.description | Under the effect of common perturbations, the multiple-soliton solution of the KdV equation is transformed into a sum of an elastic and a first-order inelastic component. The elastic component is a perturbation series, identical in structure to the perturbed single-soliton solution. It preserves the soliton-scattering picture. The inelastic component is generated by perturbation terms that represent coupling between KdV solitons and inelastically generated soliton-anti-soliton waves. It asymptotes into solitons and anti-solitons, that evolve along the characteristic lines of the KdV solitons. This is demonstrated in the two-soliton case. | |
| dc.identifier | https://arxiv.org/abs/0710.0467 | |
| dc.identifier | http://arxiv.org/abs/0710.0467 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/139161 | |
| dc.subject | Pattern Formation and Solitons | |
| dc.title | Inelastically generated solitons and anti-solitons in the perturbed KdV equation | |
| dc.type | text |