High efficiency mid-infrared 3.8 μm MgO:PPLN optical parametric oscillator pumped by narrow linewidth 1064 nm fiber laser
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摘要:采用放大1064 nm掺镱光纤 器作为泵浦源，实现了中红外3.8 μm MgO:PPLN 光参量振荡（OPO） 输出。在泵浦源中，采用分布式反馈 器（DFB）作为种子源来实现光纤 窄线宽的调制，实现线宽2.5 nm到0.1 nm的压缩，最大平均输出功率可达40 W。进一步对不同泵浦线宽条件下中红外3.8 μm MgO:PPLN OPO 进行研究，最终在泵浦功率为18.1 W、线宽为0.1 nm、重频为1 MHz、脉宽为2 ns时，获得了最高平均输出功率为2.06 W的3822.5 nm 输出，光-光转换效率为11.38%，光束质量为 M 2=2.34，提高了窄线宽泵浦对中红外MgO:PPLN OPO 输出效率。Abstract:In this paper, a 1064 nm ytterbium-doped fiber laser with Main Oscillation Power Amplification (MOPA) was used as the pump source to achieve mid-infrared 3.8 μm MgO:PPLN Optical Parametric Oscillation (OPO) laser output. In the pump source, the Distributed Feedback Laser (DFB) was used as the seed source to realize the modulation of the narrow linewidth of the fiber laser. The linewidth of 2.5 nm was compressed to 0.1 nm, and the maximum output power was 40 W. The mid-infrared 3.8 μm MgO:PPLN OPO laser was researched under different pump linewidths. Finally, when the pump power was 18.1 W, the line width was 0.1 nm, the repetition frequency was 1 MHz, and the pulse width was 2 ns, the output laser with the maximum power of 2.06 W and the wavelength of 3822.5 nm was achieved. The corresponding optical-optical conversion efficiency is 11.38%, and the beam quality is M 2= 2.34. This research can efficiency improve the output efficiency of narrow linewidth pumped mid-infrared MgO:PPLN OPO.
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Key words:
- fiber laser/
- MgO:PPLN/
- optical parametric oscillator
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图 1不同泵浦光线宽下闲频光线宽展宽与闲频光波长的关系曲线
Figure 1.Relationship between idle light broadening and idle wavelength under different pump light linewidthes
图 31064 nm掺镱光纤 器泵浦的MgO:PPLN OPO实验装置示意图
Figure 3.Schematic diagram of MgO:PPLN OPO laser pumped by 1064 nm ytterbium-doped fiber laser
图 41064 nm掺镱光纤 器输出光谱对比图
Figure 4.Comparison of output spectrum of the 1064 nm ytterbium-doped fiber laser
图 5不同线宽下1064 nm掺镱光纤 器的平均输出功率对比图
Figure 5.Comparison of output power of the 1064 nm ytterbium-doped fiber laser with different linewidths
图 6窄线宽1064 nm掺镱光纤 光束质量
Figure 6.Beam quality of the narrow linewidth 1064 nm ytterbium-doped fiber laser
图 7不同线宽1064 nm掺镱光纤 泵浦MgO:PPLN OPO平均输出功率
Figure 7.The output powers of MgO:PPLN OPO pumped by 1064 nm ytterbium-doped fiber laser with different linewidths
图 8窄线宽1064 nm掺镱光纤 泵浦MgO:PPLN OPO输出光谱图
Figure 8.The output spectrum of MgO:PPLN OPO pumped by the narrow linewidth 1064 nm ytterbium-doped fiber laser
图 9MgO:PPLN OPO 3.8 μm 输出脉冲序列和脉冲宽度图
Figure 9.Pulse sequence and pulse width of the MgO:PPLN OPO 3.8 μm laser
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[1] LIPPERT E, FONNUM H, ARISHOLM G,et al. A 22-watt mid-infrared optical parametric oscillator with V-shaped 3-mirror ring resonator[J].Optics Express, 2010, 18(25): 26475-16483.doi:10.1364/OE.18.026475 [2] LIU J, LIU Q, YAN X,et al. High repetition frequency PPMgOLN mid-infrared optical parametric oscillator[J].Laser Physics Letters, 2010, 7(9): 630-633.doi:10.1002/lapl.201010040 [3] 曾怡帅, 杨友良, 马翠红. 有尘环境多组分气体成分检测系统的设计[J]. 发光学报,2016,37(7):859-865.doi:10.3788/fgxb20163707.0859ZENG Y SH, YANG Y L, MA C H. Design of the detection system of multi component gas composition in dust environment[J].Chinese Journal of Luminescence, 2016, 37(7): 859-865. (in Chinese)doi:10.3788/fgxb20163707.0859 [4] 刘俊池, 李洪文, 王建立, 等. 中波红外整层大气透过率测量及误差分析[J]. 光学 精密工程,2015,23(6):1547-1557.doi:10.3788/OPE.20152306.1547LIU J CH, LI H W, WANG J L,et al. Measurement of mid-infrared total atmospheric transmittance and its error analysis[J].Optics and Precision Engineering, 2015, 23(6): 1547-1557. (in Chinese)doi:10.3788/OPE.20152306.1547 [5] 姚江宏, 刘志伟, 薛亮平, 等. 低阈值温度调谐PPMgLN红外光参量振荡[J]. 发光学报,2007,28(1):18-22.doi:10.3321/j.issn:1000-7032.2007.01.004YAO J H, LIU ZH W, XUE L P,et al. Low-threshold and temperature tunable optical parametrical oscillator based on periodically poled MgO:LiNbO3crystal[J].Chinese Journal of Luminescence, 2007, 28(1): 18-22. (in Chinese)doi:10.3321/j.issn:1000-7032.2007.01.004 [6] 于永吉, 陈薪羽, 成丽波, 等. 基于MgO:APLN的1.57 μm/3.84 μm连续波内腔多光参量振荡器研究[J]. 物理学报,2015,64(22):224215.doi:10.7498/aps.64.224215YU Y J, CHEN X Y, CHENG L B,et al. Continuous-wave 1.57 µm/3.84 µm intra-cavity multiple optical parametric oscillator based on MgO:APLN[J].Acta Physica Sinica, 2015, 64(22): 224215. (in Chinese)doi:10.7498/aps.64.224215 [7] SHENG Q, DING X, SHANG C,et al. Continuous-wave intra-cavity singly resonant optical parametric oscillator with resonant wave output coupling[J].Optics Express, 2012, 20(25): 27953-27958.doi:10.1364/OE.20.027953 [8] 苏辉, 李志平, 段延敏, 等. 基于掺镁周期极化铌酸锂晶体的内腔单共振连续可调谐光参量振荡器[J]. 光学 精密工程,2013,21(6):1404-1409.doi:10.3788/OPE.20132106.1404SU H, LI ZH P, DUAN Y M,et al. Intra-cavity singly resonant optical parametric oscillator based on magnesium-doped periodically poled lithium niobate[J].Optics and Precision Engineering, 2013, 21(6): 1404-1409. (in Chinese)doi:10.3788/OPE.20132106.1404 [9] 尉鹏飞, 张永昶, 张静, 等. 三镜直腔结构MgO:PPLN高效连续光参量振荡器[J]. 光学 精密工程,2019,27(1):45-50.doi:10.3788/OPE.20192701.0045WEI P F, ZHANG Y CH, ZHANG J,et al. Efficient continuous-wave MgO:PPLN optical parametric oscillator with three-mirror linear cavity[J].Optics and Precision Engineering, 2019, 27(1): 45-50. (in Chinese)doi:10.3788/OPE.20192701.0045 [10] 张雪霞, 葛廷武, 丁星, 等. 分布式抽运连续光纤 器研究[J]. 发光学报,2016,37(9):1071-1075.doi:10.3788/fgxb20163709.1071ZHANG X X, GE T W, DING X,et al. Study of continuous fiber laser with distributed pump structure[J].Chinese Journal of Luminescence, 2016, 37(9): 1071-1075. (in Chinese)doi:10.3788/fgxb20163709.1071 [11] LI J F, LUO H Y, WANG L L,et al. Tunable Fe2+: ZnSe passively Q-switched Ho3+-doped ZBLAN fiber laser around 3 μm[J].Optics Express, 2015, 23(17): 22362-22370.doi:10.1364/OE.23.022362 [12] WEI CH, LUO H Y, ZHANG H,et al. Passively Q-switched mid-infrared fluoride fiber laser around 3 µm using a tungsten disulfide (WS2) saturable absorber[J].Laser Physics Letters, 2016, 13(10): 105108.doi:10.1088/1612-2011/13/10/105108 [13] JIANG P P, CHEN T, YANG D ZH,et al. A fiber laser pumped dual-wavelength mid-infrared optical parametric oscillator based on aperiodically poled magnesium oxide doped lithium niobate[J].Laser Physics Letters, 2013, 10(11): 115405.doi:10.1088/1612-2011/10/11/115405 [14] MURRAY R T, RUNCORN T H, GUHA S,et al. High average power parametric wavelength conversion at 3.31-3.48 μm in MgO:PPLN[J].Optics Express, 2017, 25(6): 6421-6430.doi:10.1364/OE.25.006421 [15] 尚亚萍. 高功率光纤 泵浦中红外光学参量振荡器研究[D]. 长沙: 国防科学技术大学, 2017.SHANG Y P. High-power fiber lasers pumped mid-infrared optical parametric oscillator[D]. Changsha: National University of Defense Technology, 2017. (in Chinese). [16] LIU Q, WANG L, CHEN H L,et al. High repetition rate, 4 μm mid-infrared generation with periodically poled magnesium-oxide-doped lithium niobate based optical parametric oscillator pumped by fiber laser[J].Applied Physics Express, 2013, 6(5): 052704.doi:10.7567/APEX.6.052704 [17] 李港. 频率的变换与扩展: 实用非线性光学技术[M]. 北京: 科学出版社, 2005.LI G.Conversion and Expansion of Laser Frequency:Practical Nonlinear Optical Technology[M]. Beijing: Science Press, 2005. (in Chinese). -
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