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A high-power cw end-pumped laser device is demonstrated with a slab crystal of Nd:GdVO4 operating at 1063nm. Diode laser stacks at 880nm are used to pump Nd:GdVO4 into emitting level 4^F3/2. The 149 W output power is presented when the absorbed pump power is 390 W and the optical-to-optieal conversion efficiency is 38.2%. When the output power is 120 W, the M^2 factors are 2.3 in both directions. Additionally, mode overlap inside the resonator is analyzed to explain the beam quality deterioration. 相似文献
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We present an 880-nm laser-diode partially end-pumped Nd:YVO4 slab cw laser with output 126.7 W by using a hybrid resonator. The slop efficiency and optical-to-optical efficiency with respect to absorbed pumping power are 73.2% and 58.7%, respectively. At the output power of 100 W, the beam propagation M2 factors are 1.1 in the unstable direction and 1.15 in the stable direction. 相似文献
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理论设计和制作了Yb:YAG陶瓷板条,通过铟砷化镓(InGaAs)二极管抽运、1030nm种子激光注入以及双程放大,在室温下实现了高功率的1030nm激光输出。种子激光注入功率为1.18kW和总抽运功率为19.98kW时,获得了5.97kW的放大激光功率,光-光转换效率约为24.0%,斜率效率为27.9%。测量了Yb:YAG陶瓷板条的透射波前,模拟了不同耦合效率和温度时的输出功率。实验结果表明,室温下Yb:YAG在高亮度抽运和高亮度种子光注入时可以实现高功率的激光输出。 相似文献
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针对结构紧凑的部分端面泵浦混合腔板条激光放大器,研究了泵浦匀化对其输出激光光束质量的改善作用。基于ZEMAX仿真软件,设计并对比分析了直接成像和波导匀化后再成像两种泵浦耦合方式对激光二极管阵列慢轴(晶体宽度)方向光强分布均匀性的影响,发现波导匀化后泵浦均匀性得到明显提升且激光二极管阵列发光坏点对泵浦成像的影响得以弱化。进一步实验验证了泵浦匀化对Innoslab激光放大器性能的改善作用:波导匀化后慢轴方向泵浦均匀度从90.6%提高到95.4%,进而使3通放大后输出激光光束质量因子M2从2.41提升到1.55,并且有效抑制了多通放大腔内的自激振荡。 相似文献
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An 880-nm laser-diode stack end-pumped cw 1342nm Nd:YVO4 slab laser with a compact positive confocal unstable-stable hybrid resonator is demonstrated. At absorbed pump power of 115 W, the output power 32.4 W is obtained. The slope efficiency and optical-to-optical conversion efficiency are 42% and 28.2%, respectively. At output power of 22 W, the stable direction M2 is 1.3 and the unstable direction M2 is 1.2. 相似文献
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We present an experimental study of a continuous-wave Nd: YVO4 laser diode-pumped directly in band at 880 nm. By using a compact positive confocal unstable-stable hybrid resonator, a maximal laser output of 170 W at 1064 nm is realized. The slope efficiency and optical-to-optical efficiency are 56.7% and 51.3%, respectively. The M2 factors in the unstable direction and in the stable direction they are 1.9 and 1.3, respectively. 相似文献
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