为实现1.06μm波长激光向人眼安全1.57μm激光的能量转移,同时在输出光束中保留原1.06μm波长的泵浦光,以得到双波长激光的混合输出。本文从光参量振荡器(OPO)的基本原理出发,对磷酸氧钛钾(KTP)晶体的光学参量振荡(OPO)获得重频双波长...为实现1.06μm波长激光向人眼安全1.57μm激光的能量转移,同时在输出光束中保留原1.06μm波长的泵浦光,以得到双波长激光的混合输出。本文从光参量振荡器(OPO)的基本原理出发,对磷酸氧钛钾(KTP)晶体的光学参量振荡(OPO)获得重频双波长激光输出的过程进行了理论分析和实验研究。采用内腔OPO(IOPO),工作在重频20 Hz下,获得了1.57μm和1.06μm双波长激光混合输出能量大于38 m J,其中1.57μm波长信号光20 m J,脉宽5 ns;1.06μm泵浦光18 m J,脉宽6 ns,并且波形未出现外腔OPO所观察到的中央凹陷,实验结果与理论分析相吻合。展开更多
A diode pumped intracavity frequency-doubled Nd: YVO<sub>4</sub> laser emitting at 671 nm with a type- Ⅱ noncritical phase-matched LBO crystal is reported. A maximum output power at 671 nm of 404 mW was o...A diode pumped intracavity frequency-doubled Nd: YVO<sub>4</sub> laser emitting at 671 nm with a type- Ⅱ noncritical phase-matched LBO crystal is reported. A maximum output power at 671 nm of 404 mW was obtained under an incident pump power of 5.16 W, with an optical-to-optical conversion efficiency up to 7.8%. The output power fluctuates less than 5% while the temperature change of the LBO crystal is maintained at ± 0.5℃ at the phase-matched temperature.展开更多
文摘为实现1.06μm波长激光向人眼安全1.57μm激光的能量转移,同时在输出光束中保留原1.06μm波长的泵浦光,以得到双波长激光的混合输出。本文从光参量振荡器(OPO)的基本原理出发,对磷酸氧钛钾(KTP)晶体的光学参量振荡(OPO)获得重频双波长激光输出的过程进行了理论分析和实验研究。采用内腔OPO(IOPO),工作在重频20 Hz下,获得了1.57μm和1.06μm双波长激光混合输出能量大于38 m J,其中1.57μm波长信号光20 m J,脉宽5 ns;1.06μm泵浦光18 m J,脉宽6 ns,并且波形未出现外腔OPO所观察到的中央凹陷,实验结果与理论分析相吻合。
文摘A diode pumped intracavity frequency-doubled Nd: YVO<sub>4</sub> laser emitting at 671 nm with a type- Ⅱ noncritical phase-matched LBO crystal is reported. A maximum output power at 671 nm of 404 mW was obtained under an incident pump power of 5.16 W, with an optical-to-optical conversion efficiency up to 7.8%. The output power fluctuates less than 5% while the temperature change of the LBO crystal is maintained at ± 0.5℃ at the phase-matched temperature.