Adaptation to the edge of chaos in a self-starting Kerr-lens mode-locked laser
| dc.citation.epage | 408 | en_US |
| dc.citation.issue | 2-3 | en_US |
| dc.citation.spage | 401 | en_US |
| dc.citation.volume | 96 | en_US |
| dc.citation.woscount | 0 | |
| dc.contributor.author | Hsu, C. C. | en_US |
| dc.contributor.author | Lin, J. H. | en_US |
| dc.contributor.author | Hsieh, W. F. | en_US |
| dc.contributor.department | 光電工程學系 | zh_TW |
| dc.contributor.department | Department of Photonics | en_US |
| dc.date.accessioned | 2014-12-08T15:08:59Z | |
| dc.date.available | 2014-12-08T15:08:59Z | |
| dc.date.issued | 2009-08-01 | en_US |
| dc.description.abstract | We experimentally and numerically demonstrated that self-focusing acts as a slow-varying control parameter that suppresses the transient chaos to reach a stable mode-locking (ML) state in a self-starting Kerr-lens mode-locked Ti:sapphire laser without external modulation and feedback control. Based on Fox-Li's approach, including the self-focusing effect, the theoretical simulation reveals that the self-focusing effect is responsible for the self-adaptation. The self-adaptation occurs at the boundary between the chaotic and continuous output regions in which the laser system begins with a transient chaotic state with fractal correlation dimension, and then evolves with reducing dimension into the stable ML state. | en_US |
| dc.identifier.doi | 10.1007/s00340-009-3539-3 | en_US |
| dc.identifier.issn | 0946-2171 | en_US |
| dc.identifier.journal | APPLIED PHYSICS B-LASERS AND OPTICS | en_US |
| dc.identifier.uri | http://dx.doi.org/10.1007/s00340-009-3539-3 | en_US |
| dc.identifier.uri | https://ir.lib.nycu.edu.tw/handle/11536/6834 | |
| dc.identifier.wosnumber | WOS:000267885000025 | |
| dc.language.iso | en_US | en_US |
| dc.title | Adaptation to the edge of chaos in a self-starting Kerr-lens mode-locked laser | en_US |
| dc.type | Article | en_US |