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COMPLETELY SELF-STARTING PICOSECOND AND FEMTOSECOND KERR-LENS MODE-LOCKED TI-SAPPHIRE LASER

dc.citation.epage949en_US
dc.citation.issue5en_US
dc.citation.spage945en_US
dc.citation.volume12en_US
dc.citation.woscount8
dc.contributor.authorSHIEH, JMen_US
dc.contributor.authorGANIKHANOV, Fen_US
dc.contributor.authorLIN, KHen_US
dc.contributor.authorHSIEH, WFen_US
dc.contributor.authorPAN, CLen_US
dc.contributor.department交大名義發表zh_TW
dc.contributor.department光電工程學系zh_TW
dc.contributor.departmentNational Chiao Tung Universityen_US
dc.contributor.departmentDepartment of Photonicsen_US
dc.date.accessioned2014-12-08T15:03:24Z
dc.date.available2014-12-08T15:03:24Z
dc.date.issued1995-05-01en_US
dc.description.abstractCompletely self-starting and stable operation of a Kerr-lens mode-locked Ti:sapphire laser was realized in both picosecond and femtosecond regimes. The cavity has a symmetric X configuration with soft aperturing. Enhanced Kerr nonlinearity and reduced backscattering effects were thought to be key to obtaining stable self-starting self-mode-locked operation from 765 to 815 nm far the picosecond regime and from 770 to 835 nm for the femtosecond regime. The mode-locking starting time as measured by the onset of the second-harmonic signal ranged from 300 ms to 2 s, depending on cavity alignment. Preliminary data also suggest that intracavity intensity fluctuation necessary for the laser to evolve into stable mode locking could be as short as 10-40 ps.en_US
dc.identifier.doi10.1364/JOSAB.12.000945en_US
dc.identifier.issn0740-3224en_US
dc.identifier.journalJOURNAL OF THE OPTICAL SOCIETY OF AMERICA B-OPTICAL PHYSICSen_US
dc.identifier.urihttp://dx.doi.org/10.1364/JOSAB.12.000945en_US
dc.identifier.urihttps://ir.lib.nycu.edu.tw/handle/11536/1953
dc.identifier.wosnumberWOS:A1995QW72500027
dc.language.isoen_USen_US
dc.titleCOMPLETELY SELF-STARTING PICOSECOND AND FEMTOSECOND KERR-LENS MODE-LOCKED TI-SAPPHIRE LASERen_US
dc.typeArticleen_US

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