Jun Meng 1Chen Li 1Zhenhua Cong 1,2,3Zhigang Zhao 1,2,3[ ... ]Zhaojun Liu 1,2,3
Author Affiliations
Abstract
1 School of Information Science and Engineering, Shandong University, Qingdao 266237, China
2 Shandong Provincial Key Laboratory of Laser Technology and Application, Qingdao 266237, China
3 Key Laboratory of Laser & Infrared System (Shandong University), Ministry of Education, Qingdao 266237, China
4 Center for Optics Research and Engineering, Shandong University, Qingdao 266237, China
A high-energy 100-Hz optical parametric oscillator (OPO) based on a confocal unstable resonator with a Gaussian reflectivity mirror was demonstrated. A KTA-based OPO with a good beam quality was obtained when the magnification factor was 1.5, corresponding to the maximum signal (1.53 µm) energy of 56 mJ and idler (3.47 µm) energy of 20 mJ, respectively. The beam quality factors (M2) were measured to be M2x = 5.7, M2y = 5.9 for signal and M2x = 8.4, M2y = 8.1 for idler accordingly. The experimental results indicated that the beam quality positively changed with the increase of magnification factors, accompanied by an acceptable loss of pulse energy.
optical parametric oscillators confocal unstable resonator beam quality 
Chinese Optics Letters
2023, 21(5): 051401
Jun Meng 1Chen Li 1Zhenhua Cong 1,2,3Zhigang Zhao 1,2,3[ ... ]Zhaojun Liu 1,2,3,*
Author Affiliations
Abstract
1 School of Information Science and Engineering, Shandong University, Qingdao 266237, China
2 Shandong Provincial Key Laboratory of Laser Technology and Application, Qingdao 266237, China
3 Key Laboratory of Laser & Infrared System (Shandong University), Ministry of Education, Qingdao 266237, China
4 Center for Optics Research and Engineering, Shandong University, Qingdao 266237, China
Beam quality improvements by a large margin for signal and idler beams of a high energy 100 Hz KTiOAsO4 (KTA) non-critical phase matching (NCPM) optical parametric oscillator (OPO) were demonstrated using an unstable resonator configuration instead of a plane-parallel one. Theoretically, influences of cavity lengths and transmission of an output coupler on the OPO conversion efficiency for both were numerically simulated. For OPO based on an unstable resonator with a Gaussian reflectivity mirror, the maximum pulse energies at the signal (1.53 µm) and idler (3.47 µm) were about 75 mJ and 26 mJ, respectively. The corresponding beam quality factors of the signal were Mx2 = 9.8 and My2 = 9.9, and Mx2 = 11.2 and My2 = 11.5 for the idler. As a comparison, 128 mJ of signal and 48 mJ of idler were obtained with the plane-parallel resonator, and the M2 factors of the signal were Mx2 = 39.8 and My2 = 38.4, and Mx2 = 32.1 and My2 = 31.4 for the idler. Compared with a plane-parallel cavity, over eight times and three times brightness improvements were realized for the signal and idler light, respectively.
optical parametric oscillators unstable resonator beam quality 
Chinese Optics Letters
2022, 20(9): 091401
作者单位
摘要
哈尔滨工业大学 可调谐激光技术国家级重点实验室,黑龙江 哈尔滨 150001
2 μm、中波红外3~5 μm及长波红外8~12 μm波段的激光处于大气传输窗口,在激光医疗、环境监测、激光雷达、化学遥感和红外对抗等领域有着非常广阔的应用前景。基于非线性频率转换技术,采用非线性光学晶体在实现中长波红外固体激光输出方面具有结构简单、宽调谐和高功率等技术优势。尤其是使用2 μm单掺Ho固体激光器泵浦ZnGeP2晶体,在3~5 μm和8~10 μm中长波红外输出中性能优异。在平均输出功率方面,目前可达到102 W@3~5 μm、12.6 W@8.2 μm以及3.5 W@9.8 μm的输出水平,光束质量M2均小于3,其中中波的光光转换效率可达60%。文中针对2 μm单掺Ho固体激光器及ZnGeP2晶体在中长波输出方面进行了总结。
中长波红外 非线性光学 固体激光器 2 μm 2 μm middle-long-wave infrared nonlinear optics solid laser 
红外与激光工程
2020, 49(12): 20201056
作者单位
摘要
哈尔滨工业大学, 可调谐激光技术国家级重点实验室, 哈尔滨 150001
中波红外3~5 μm波段以及长波红外8~12 μm波段的激光处于大气传输窗口, 在激光成像、环境监测、激光雷达、激光医疗、化学遥感和红外对抗等领域有着非常广阔的应用前景。基于非线性光学晶体, 采用光学非线性频率变换技术在实现中长波红外固体激光输出方面具有明显的技术优势。该方法激光器结构简单, 且晶体本身并不参与能量交换, 因而没有量子亏损, 从而产热很少。同时具有单色性好、宽调谐、高功率等优点。本文针对常用以及新型非线性光学晶体, 对其应用于中长波红外固体激光器的研究进展做了详细的总结。
中长波红外激光 固体激光器 非线性光学晶体 光学非线性频率变换技术 mid- and long-wave infrared laser solid-state laser nonlinear optical crystal optical nonlinear frequency conversion technology 
人工晶体学报
2020, 49(8): 1379
Author Affiliations
Abstract
National Key Laboratory of Tunable Laser Technology, Harbin Institute of Technology, Harbin 150001, China
We demonstrate a Fe:ZnSe laser gain-switched by a ZnGeP2 optical parametric oscillator (OPO) under the pulse repetition frequency of 1 kHz at room temperature. The 2.9 μm signal light of the OPO is employed as the pump for the Fe:ZnSe laser. The maximum output power of the Fe:ZnSe laser is 58 mW with the pulse duration of 2.7 ns under the incident pump power of 280 mW, corresponding to a peak pulse power of 21.5 kW and an optical-to-optical efficiency of 20.7%. The spectrum of the Fe:ZnSe laser has a range of 4030.2–4593.6 nm with a dip at 4187.1–4340.4 nm due to the absorption of CO2.
140.3070 Infrared and far-infrared lasers 140.3295 Laser beam characterization 
Chinese Optics Letters
2019, 17(8): 081404
刘高佑 1,2,*安宁 1韩兴伟 1董雪 1[ ... ]刘承志 1
作者单位
摘要
1 中国科学院国家天文台 长春人造卫星观测站, 吉林 长春 130117
2 中国科学院大学, 北京 100049
利用有限元光腔表面分割法对立方腔的平均反射光程(Average Reflex Optical Path Length, Lave)进行了数值模拟, 给出了Lave与腔长的线性关系式, 并通过TDLAS实验得到了具有不同腔长的立方腔Lave的实验值。研究结果表明, 立方腔的Lave随着腔长的增加而线性增大。与之前报道的理论结果相比, 采用有限元光腔表面分割法得到的Lave模拟值与实验值更为接近, 误差率仅在2.5%以内。立方腔平均反射光程模拟值与腔长的关系可以作为确定腔长的依据, 提高了基于立方腔的TDLAS气体测量系统的反演精度。
有限元光腔表面分割法 数值模拟 Lave Lave finite element cavity surface segmentation TDLAS TDLAS numerical simulation 
红外与激光工程
2016, 45(11): 1118003

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