The preferable resonators for Kerr-lens mode-locking determined by stability factors of their iterative maps
| dc.citation.epage | 412 | en_US |
| dc.citation.spage | 406 | en_US |
| dc.citation.volume | 155 | en_US |
| dc.citation.woscount | 6 | en_US |
| dc.contributor.author | Wei, MD | en_US |
| dc.contributor.author | Hsieh, WF | en_US |
| dc.contributor.author | Sung, CC | en_US |
| dc.contributor.department | 光電工程研究所 | zh_TW |
| dc.contributor.department | Institute of EO Enginerring | en_US |
| dc.date.accessioned | 2019-04-02T05:59:32Z | |
| dc.date.available | 2019-04-02T05:59:32Z | |
| dc.date.issued | 1998-10-15 | en_US |
| dc.description.abstract | The generalized stability factor of a general resonator was obtained from its iterative map based on the linear stability analysis. Since a physical system tends to stay with high stability, the preferred resonator for Kerr-lens mode-locking (KLM) is determined by the relative stability between KLM and CW operations. With this criterion the preferable KLM regions agree with the previous experimental self-starting regions when the Ken medium is located around the center of the resonator. (C) 1998 Elsevier Science B.V. All rights reserved. | en_US |
| dc.identifier.doi | 10.1016/S0030-4018(98)00374-5 | en_US |
| dc.identifier.issn | 0030-4018 | en_US |
| dc.identifier.journal | OPTICS COMMUNICATIONS | en_US |
| dc.identifier.uri | http://dx.doi.org/10.1016/S0030-4018(98)00374-5 | en_US |
| dc.identifier.uri | https://ir.lib.nycu.edu.tw/handle/11536/150492 | |
| dc.identifier.wosnumber | WOS:000076602200030 | en_US |
| dc.language.iso | en_US | en_US |
| dc.subject | resonators | en_US |
| dc.subject | Kerr-lens mode-locking | en_US |
| dc.subject | iterative maps | en_US |
| dc.subject | linear stability analysis | en_US |
| dc.title | The preferable resonators for Kerr-lens mode-locking determined by stability factors of their iterative maps | en_US |
| dc.type | Article | en_US |
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