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EFFECT OF DYE CONCENTRATION ON PICOSECOND AND FEMTOSECOND CW PASSIVELY MODE-LOCKED TI-SAPPHIRE DDI LASERS

dc.citation.epage1446en_US
dc.citation.issue20en_US
dc.citation.spage1444en_US
dc.citation.volume17en_US
dc.citation.woscount5
dc.contributor.authorPAN, CLen_US
dc.contributor.authorHWANG, CDen_US
dc.contributor.authorKUO, JCen_US
dc.contributor.authorSHIEH, JMen_US
dc.contributor.authorWU, KHen_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.department光電工程學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.contributor.departmentDepartment of Photonicsen_US
dc.date.accessioned2014-12-08T15:04:45Z
dc.date.available2014-12-08T15:04:45Z
dc.date.issued1992-10-15en_US
dc.description.abstractThe role of the saturable absorber dye DDI in the cw passively mode-locked Ti:sapphire/DDI laser both with and without compensation prisms is investigated. This laser self-starts when the concentration of the dye is greater than almost-equal-to 2 X 10(-4) M for both picosecond and femtosecond pulses. With the prism pair, the laser generates Gaussian pulses 150 fs in duration. The corresponding spectrum is sech2 in shape with a FWHM of 8 nm. These parameters are independent of the DDI concentration. Without the prism pair, the laser generates picosecond pulses with the FWHM decreasing from 8 to 3 ps as the dye concentration is increased from 2.5 x 10(-4) to 1 X 10(-3) M. Concurrently the pulse shape changes from a Lorentzian to a nearly symmetric two-sided exponential shape. The picosecond spectra for different dye concentrations are also presented.en_US
dc.identifier.doi10.1364/OL.17.001444en_US
dc.identifier.issn0146-9592en_US
dc.identifier.journalOPTICS LETTERSen_US
dc.identifier.urihttp://dx.doi.org/10.1364/OL.17.001444en_US
dc.identifier.urihttps://ir.lib.nycu.edu.tw/handle/11536/3265
dc.identifier.wosnumberWOS:A1992JT56800015
dc.language.isoen_USen_US
dc.titleEFFECT OF DYE CONCENTRATION ON PICOSECOND AND FEMTOSECOND CW PASSIVELY MODE-LOCKED TI-SAPPHIRE DDI LASERSen_US
dc.typeArticleen_US

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