Full metadata record
DC Field | Value | Language |
---|---|---|
dc.contributor.author | Wang, J. -Y. | en_US |
dc.contributor.author | Lin, K. -H. | en_US |
dc.contributor.author | Chen, H. -R. | en_US |
dc.date.accessioned | 2014-12-08T15:21:33Z | - |
dc.date.available | 2014-12-08T15:21:33Z | - |
dc.date.issued | 2012-01-01 | en_US |
dc.identifier.issn | 1054-660X | en_US |
dc.identifier.uri | http://dx.doi.org/10.1134/S1054660X11230198 | en_US |
dc.identifier.uri | http://hdl.handle.net/11536/15315 | - |
dc.description.abstract | Passive optical waveform generation is obtained in fiber lasers using a 1.3-mu m semiconductor optical amplifier (SOA) as the gain medium. Various waveforms, including square wave, staircase wave, triangular wave, pulse, and dark pulse are generated in SOA-based fiber lasers by adjusting intracavity polarization controllers. The passive waveform generation might be attributed to the SOA gain dynamics and the enhanced nonlinear interaction at the 1.3-mu m zero dispersion wavelength of traditional single-mode fiber (SMF), as well as the interference effect between the two sub-cavities of fiber laser. With figure-8 cavity configuration, 1250th-order harmonic pulses have been successfully demonstrated. We have also obtained a free-running SOA-based fiber laser with 3-dB spectral width of 16 nm, and the center wavelength can be tuned over 45 nm range. | en_US |
dc.language.iso | en_US | en_US |
dc.title | Generation of optical waveforms in 1.3-mu m SOA-based fiber lasers | en_US |
dc.type | Article | en_US |
dc.identifier.doi | 10.1134/S1054660X11230198 | en_US |
dc.identifier.journal | LASER PHYSICS | en_US |
dc.citation.volume | 22 | en_US |
dc.citation.issue | 1 | en_US |
dc.citation.spage | 216 | en_US |
dc.citation.epage | 220 | en_US |
dc.contributor.department | 光電工程學系 | zh_TW |
dc.contributor.department | Department of Photonics | en_US |
dc.identifier.wosnumber | WOS:000298994000033 | - |
dc.citation.woscount | 4 | - |
Appears in Collections: | Articles |
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