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dc.contributor.authorCheng, H. P.en_US
dc.contributor.authorHuang, T. L.en_US
dc.contributor.authorLee, C. Y.en_US
dc.contributor.authorSung, C. L.en_US
dc.contributor.authorCho, C. Y.en_US
dc.contributor.authorChen, Y. F.en_US
dc.date.accessioned2019-04-03T06:37:24Z-
dc.date.available2019-04-03T06:37:24Z-
dc.date.issued2016-10-17en_US
dc.identifier.issn1094-4087en_US
dc.identifier.urihttp://dx.doi.org/10.1364/OE.24.023829en_US
dc.identifier.urihttp://hdl.handle.net/11536/132881-
dc.description.abstractThe self-mode-locked (SML) operation at 946 nm can be achieved with a monolithic Nd: YAG crystal when the pump power is above the threshold of the multiple-longitudinal-mode generation. The SML output is further found to include two orthogonal polarization components with a beat frequency coming from the birefringence effect in the laser crystal. The beat frequency can be widely adjusted in the range of 5-220 MHz by controlling the cooling temperature. The present experiment also confirms the theoretical prediction that the two-mode operation generally exhibits the chaotic dynamics when the frequency difference is sufficiently close to the relaxation frequency. (C) 2016 Optical Society of Americaen_US
dc.language.isoen_USen_US
dc.titleMonolithic dual-polarization self-mode-locked Nd: YAG 946-nm lasers: controlling beat frequency and observation of temporal chaosen_US
dc.typeArticleen_US
dc.identifier.doi10.1364/OE.24.023829en_US
dc.identifier.journalOPTICS EXPRESSen_US
dc.citation.volume24en_US
dc.citation.issue21en_US
dc.citation.spage23829en_US
dc.citation.epage23837en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:000388399100019en_US
dc.citation.woscount6en_US
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