完整後設資料紀錄
DC 欄位語言
dc.contributor.authorWei, MDen_US
dc.contributor.authorHsieh, WFen_US
dc.contributor.authorSung, CCen_US
dc.date.accessioned2019-04-02T05:59:32Z-
dc.date.available2019-04-02T05:59:32Z-
dc.date.issued1998-10-15en_US
dc.identifier.issn0030-4018en_US
dc.identifier.urihttp://dx.doi.org/10.1016/S0030-4018(98)00374-5en_US
dc.identifier.urihttp://hdl.handle.net/11536/150492-
dc.description.abstractThe 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.language.isoen_USen_US
dc.subjectresonatorsen_US
dc.subjectKerr-lens mode-lockingen_US
dc.subjectiterative mapsen_US
dc.subjectlinear stability analysisen_US
dc.titleThe preferable resonators for Kerr-lens mode-locking determined by stability factors of their iterative mapsen_US
dc.typeArticleen_US
dc.identifier.doi10.1016/S0030-4018(98)00374-5en_US
dc.identifier.journalOPTICS COMMUNICATIONSen_US
dc.citation.volume155en_US
dc.citation.spage406en_US
dc.citation.epage412en_US
dc.contributor.department光電工程研究所zh_TW
dc.contributor.departmentInstitute of EO Enginerringen_US
dc.identifier.wosnumberWOS:000076602200030en_US
dc.citation.woscount6en_US
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