4.6 Article

Stability of solitary waves in nonlinear Klein-Gordon equations

出版社

IOP Publishing Ltd
DOI: 10.1088/1751-8121/aca0d1

关键词

nonlinear Klein-Gordon equations; Sturm-Liouville problem; stability; kink solution

资金

  1. FEDER(EU)/Ministerio de Ciencia e Innovacion-Agencia Estatal de Investigacion [PGC2018-096504-B-C31]
  2. FEDET(EU)-Junta de Andalucia [FQM-262, Feder-US-1254600]
  3. MICIN [PID2020-113390GB-I00]
  4. Junta de Andalucia [PY20_00082]
  5. ERDF-University of Granada [A-FQM-52-UGR20]
  6. Andalusian research Group [FQM-207]

向作者/读者索取更多资源

The stability of topological solitary waves and pulses in one-dimensional nonlinear Klein-Gordon systems is investigated. The linearized equation leads to a Sturm-Liouville problem, which is systematically solved for the l(l+1)sech(2)(x) potential, demonstrating the orthogonality and completeness of the solution set. Two families of novel nonlinear Klein-Gordon potentials are introduced, and their exact solutions are calculated even when the nonlinear potential is unknown. It is found that the kinks of the novel models are stable, while the pulses are unstable unless certain spatial inhomogeneities are introduced.
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)sech(2)(x)-potential, showing the orthogonality and completeness relations fulfilled by the set of its solutions for all values l is an element of N. This approach allows to determine the linear stability of kinks and pulses of certain nonlinear Klein-Gordon equations. Two families of novel nonlinear Klein-Gordon potentials are introduced. The exact solutions (kinks and pulses) for these potentials are exactly calculated, even when the nonlinear potential is not explicitly known. The kinks of the novel models 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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