Stability of solitary waves in nonlinear Klein-Gordon equations
The stability of topological solitary waves and pulses in one-dimensional nonlinear Klein–Gordon systems is revisited. The linearized equation describing small deviations around the static solution leads to a Sturm–Liouville problem, which is solved in a systematic way for the -l(l+1)sech2(x), showi...
| Autores: | , , |
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| Tipo de documento: | artigo |
| Estado: | Versión enviada para evaluación y publicación |
| Data de publicação: | 2022 |
| País: | España |
| Recursos: | Universidad de Sevilla (US) |
| Repositório: | idUS. Depósito de Investigación de la Universidad de Sevilla |
| OAI Identifier: | oai:idus.us.es:11441/140576 |
| Acesso em linha: | https://hdl.handle.net/11441/140576 https://doi.org/10.1088/1751-8121/aca0d1 |
| Access Level: | Acceso aberto |
| Palavra-chave: | Nonlinear Klein–Gordon equations Sturm–Liouville problem Stability Kink solution |
| Resumo: | The stability of topological solitary waves and pulses in one-dimensional nonlinear Klein–Gordon systems is revisited. The linearized equation describing small deviations around the static solution leads to a Sturm–Liouville problem, which is solved in a systematic way for the -l(l+1)sech2(x), showing the orthogonality and completeness relations fulfilled by the set of its solutions for all values l Ɛ N. This approach enables the linear stability of kinks and pulses of certain nonlinear Klein–Gordon equations to be determined. The inverse problem, which starts from Sturm–Liouville problem and obtains nonlinear Klein–Gordon potentials, is also revisited and solved in a direct way. The exact solutions (kinks and pulses) for these potentials are calculated, even when the nonlinear potential is not explicitly known. The kinks are found to be stable, whereas the pulses are unstable. The stability of the pulses is achieved by introducing certain spatial inhomogeneities. |
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