Browsing by Author "Chang, Teng-Yao"
Now showing 1 - 2 of 2
- Results Per Page
- Sort Options
Item type:Item, High-power, passively mode-locked Nd:GdVO(4) laser using single-walled carbon nanotubes as saturable absorber(2011-04-01) ;Chen, Hou-Ren ;Wang, Yong-Gang ;Tsai, Chih-Ya ;Lin, Kuei-HueiChang, Teng-YaoWe use a new (to our knowledge) fabrication method of a single-walled carbon nanotube (SWCNT) absorber without polymer to sustain high-power illumination. Using a series of saturable absorbers (SAs) incorporating different amounts of SWCNTs, we demonstrate mode-locking for a Nd:GdVO(4) laser in the 1 mu m spectral range. Continuous-wave mode-locking (CWML) pulses with a maximum output power of 3.6 W at 1063 nm and high noise extinction of 61 dB has been achieved to give the highest pulse peak power of 3.6 kW and pulse energy of 30 nJ under 15 W pumping. To our knowledge, this is the highest CWML output power with SWCNT-SAs reported. The measured nonlinear absorption of the SWCNT-SAs shows a modulation depth of similar to 3% with subpicosecond recovery time. (C) 2011 Optical Society of AmericaItem type:Item, High-power, passively mode-locked Nd:GdVO4 laser using single-walled carbon nanotubes as saturable absorber(2011-04-01) ;Chen, Hou-Ren ;Wang, Yong-Gang ;Tsai, Chih-Ya ;Lin, Kuei-HueiChang, Teng-YaoWe use a new (to our knowledge) fabrication method of a single-walled carbon nanotube (SWCNT) absorber without polymer to sustain high-power illumination. Using a series of saturable absorbers (SAs) incorporating different amounts of SWCNTs, we demonstrate mode-locking for a Nd:GdVO4 laser in the 1 mu m spectral range. Continuous-wave mode-locking (CWML) pulses with a maximum output power of 3.6 W at 1063 nm and high noise extinction of 61 dB has been achieved to give the highest pulse peak power of 3.6 kW and pulse energy of 30 nJ under 15 W pumping. To our knowledge, this is the highest CWML output power with SWCNT-SAs reported. The measured nonlinear absorption of the SWCNT-SAs shows a modulation depth of similar to 3% with subpicosecond recovery time. (C) 2011 Optical Society of America