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dc.contributor.authorGuo, L.en_US
dc.contributor.authorWang, G. L.en_US
dc.contributor.authorZhang, H. B.en_US
dc.contributor.authorCui, D. F.en_US
dc.contributor.authorWu, Y. C.en_US
dc.contributor.authorLu, L.en_US
dc.contributor.authorZhang, J. Y.en_US
dc.contributor.authorHuang, J. Y.en_US
dc.contributor.authorXu, Z. Y.en_US
dc.date.accessioned2014-12-08T15:13:40Z-
dc.date.available2014-12-08T15:13:40Z-
dc.date.issued2007-07-01en_US
dc.identifier.issn0946-2171en_US
dc.identifier.urihttp://dx.doi.org/10.1007/s00340-007-2713-8en_US
dc.identifier.urihttp://hdl.handle.net/11536/10575-
dc.description.abstractWe report on the high average power third harmonic generation (THG) of a mode-locked picosecond laser in a CsB3O5 (CBO) crystal. The picosecond laser beam at 1064 nm is produced by a home-made 30 W master oscillator power-amplifier (MOPA) Nd:YVO4 laser system. The maximum THG output at 355 nm is up to 5.4 W. We also investigate the phase matching angle at different temperatures. During high power operation, the temperature of the CBO crystal is set at a high temperature of more than 100 degrees C. The THG system has shown a fine long-term stability for more than two months of operation.en_US
dc.language.isoen_USen_US
dc.titleHigh-power picoseconds 355 nm laser by third harmonic generation based on CsB3O5 crystalen_US
dc.typeArticleen_US
dc.identifier.doi10.1007/s00340-007-2713-8en_US
dc.identifier.journalAPPLIED PHYSICS B-LASERS AND OPTICSen_US
dc.citation.volume88en_US
dc.citation.issue2en_US
dc.citation.spage197en_US
dc.citation.epage200en_US
dc.contributor.department光電工程學系zh_TW
dc.contributor.departmentDepartment of Photonicsen_US
dc.identifier.wosnumberWOS:000248054900008-
dc.citation.woscount14-
Appears in Collections:Articles


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