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Ho∶YLF激光泵浦的长波红外ZnGeP2光参量振荡器

Long-Wave Infrared ZnGeP2 Optical Parametric Oscillator Pumped by Ho∶YLF Laser

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摘要

以2.05μm Ho∶YLF激光器作为光源,泵浦了长波ZnGeP2 光参量振荡器,实现了高效率、高重复频率的长波激光输出。激光器输出的峰值波长为8.1μm,最大输出功率为3.2W@10kHz,泵浦激光到长波激光的光光转换效率为12%,斜效率为19.3%,激光单脉冲宽度为27.11ns,单脉冲能量为0.32mJ,单脉冲峰值功率为11.8kW,X方向的光束质量因子为4.5,Y方向的光束质量因子为4.2。

Abstract

Objective The 8--12μm long-wave infrared laser is just within the transmission bands of atmosphere and widely used for gas composition detection and electro-optic countermeasure. As traditional long-wave lasers, CO2 lasers can output lasers with a specific wavelength within the range of 9--10μm. Beyond them, a long-wave infrared optical parametric oscillator (OPO) shows an enormous advantage because of its wavelength tuning. However, OPO-based lasers with wavelengths longer than 8μm and high optical-to-optical conversion efficiency are still scarce. Herein, we construct a ZnGeP2 OPO and experimentally test its long-wave infrared output. The experimental result shows that a long-wave laser with high conversion efficiency is obtained, which provides a reference to engineer the laser based on ZnGeP2 OPO.

Methods The scheme of the OPO-based long-wave infrared laser pumped by a 2μm laser is discussed, in which the selection of a 2μm laser crystal and a long-wave infrared nonlinear crystal is included. In this scheme, the selected nonlinear crystal is ZnGeP2, and the selected pumping laser source is 2.05μm Ho∶YLF laser with a maximum output power of 27W (10kHz). The two end faces of the ZnGeP2 crystal are polished and coated with an antireflection film at 2.05, 2.7, and 8.2μm bands, which are the key processes for reducing the optical loss in the crystal and for reducing the risk of damage. The resonator of the ZnGeP2 OPO is a flat cavity and the resonant mode is double resonance OPO. The Ho∶YLF laser is linearly polarized, which is helpful for ZnGeP2 OPOs to achieve a high optical-to-optical conversion efficiency. The Ho∶YLF laser, pulsed using an acousto-optic Q-switch, is pumped by a Tm∶YAP laser (CW) with a wavelength of 1.94μm and a maximum output power of 62W. Without damaging the elements of the Ho∶YLF laser, the laser’s repetition rate is minimized, the OPO’s threshold is reduced, and the conversion efficiency is improved. The ZnGeP2 crystal, Ho∶YLF crystal, and Tm∶YAP crystal are all wrapped in thin indium foils and placed in copper heat sinks to collect the heat absorbed by them. During the operation of the experimental apparatus, there is the water flow with 20 ℃ in the Q-switch and all heat sinks, and a microchannel structure for the water flow is indicated. Finally, the typical parameters of the long-wave infrared laser, including average power, wavelength, laser beam quality, repetition rate, and pulse duration, are measured.

Results and Discussions The laser experimental apparatus (corresponding to the scheme mentioned above) achieves good experimental results with high power, efficiency, and repetition rate. The long-wave laser is generated when the 2.05μm pulsed laser with an average power of 10.5W is injected. The maximum output power of the long-wave laser is 3.2W when the 2.05μm pulsed laser with an average power of 26.68W is injected. Meanwhile, the corresponding optical-to-optical conversion efficiency is up to 12% and the slope efficiency is up to 19.3%. A spectrum analyzer is used to measure the spectrum of the long-wave laser with an output power of 3.2W and the peak wavelength of 8.135μm is disclosed. A CCD laser beam analyzer is used to measure the laser beam quality factor of the long-wave laser with an output power of 3.2W. The focusing lens method is used for these measurements. After the measurements, the quality factor is 4.5 in the X direction and 4.2 in the Y direction. The laser parameters including repetition rate of 10kHz and pulse duration of 27.11ns are measured using a photoelectric detector. The simple calculation shows that the single pulse laser energy is 0.32mJ and the peak power is 11.8kW.

Conclusions We verify that a ZnGeP2 OPO is feasible to realize high efficiency and tunable long-wave laser output. First, the phase-matching mode and the phase-matching angle of the ZnGeP2 crystal are analyzed and designed according to the principle that the output laser wavelength of a ZnGeP2 OPO corresponds to its phase-matching angle. Second, to realize the 8μm laser, the ZnGeP2 crystal is processed according to the above phase-matching angle. Third, the experimental apparatus is set up and the effect of the long-wave ZnGeP2 OPO laser is verified, and the ZnGeP2 OPO laser pumped by the 2.05μm Ho∶YLF pulsed laser can generate a long-wave laser output with a specific wavelength, high efficiency, and high power. In the future, long-wave infrared lasers with wavelengths longer than 8μm can be achieved just by reducing the phase-matching angle of the ZnGeP2 crystal (changing its cutting angle as an example) or reducing the incident angle of the pump laser.

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中图分类号:TN248.1

DOI:10.3788/CJL202148.0101002

所属栏目:激光器件与激光物理

基金项目:中国科学院大气光学重点实验室开放课题基金;

收稿日期:2020-06-15

修改稿日期:2020-08-24

网络出版日期:2021-01-01

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魏磊:中国科学院安徽光学精密机械研究所中国科学院大气光学重点实验室, 安徽 合肥 230031中国科学技术大学研究生院科学岛分院, 安徽 合肥 230026先进激光技术安徽省实验室, 安徽 合肥 230037华北光电技术研究所固体激光技术重点实验室, 北京 100015
吴德成:中国科学院安徽光学精密机械研究所中国科学院大气光学重点实验室, 安徽 合肥 230031先进激光技术安徽省实验室, 安徽 合肥 230037
刘东:中国科学院安徽光学精密机械研究所中国科学院大气光学重点实验室, 安徽 合肥 230031先进激光技术安徽省实验室, 安徽 合肥 230037
赵书云:华北光电技术研究所固体激光技术重点实验室, 北京 100015
陈国:华北光电技术研究所固体激光技术重点实验室, 北京 100015
李宝:华北光电技术研究所固体激光技术重点实验室, 北京 100015
方聪:华北光电技术研究所固体激光技术重点实验室, 北京 100015
韩隆:华北光电技术研究所固体激光技术重点实验室, 北京 100015
王英俭:中国科学院安徽光学精密机械研究所中国科学院大气光学重点实验室, 安徽 合肥 230031先进激光技术安徽省实验室, 安徽 合肥 230037

联系人作者:王英俭(wyj@aiofm.ac.cn)

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引用该论文

Wei Lei,Wu Decheng,Liu Dong,Zhao Shuyun,Chen Guo,Li Bao,Fang Cong,Han Long,Wang Yingjian. Long-Wave Infrared ZnGeP2 Optical Parametric Oscillator Pumped by Ho∶YLF Laser[J]. Chinese Journal of Lasers, 2021, 48(1): 0101002

魏磊,吴德成,刘东,赵书云,陈国,李宝,方聪,韩隆,王英俭. Ho∶YLF激光泵浦的长波红外ZnGeP2光参量振荡器[J]. 中国激光, 2021, 48(1): 0101002

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