作者单位
摘要
江苏师范大学 物理与电子工程学院,江苏 徐州 221116
基于固体介质的拉曼频率变换是产生新波段激光的有效技术方案。利用1572 nm KTP光参量振荡器腔内泵浦KGW晶体,实现了1616 nm (2阶)、1638 nm (3阶)、1662 nm (4阶)、1686 nm (5阶)、1711 nm (6阶)拉曼激光输出,其中1711 nm占据主导地位。激光器最大总平均输出功率为1.13 W,最小脉冲宽度为20 ns。该多阶级联拉曼变频对应的单阶平均拉曼频移为86 cm−1,与文献报道的KGW晶体低频拉曼模式相吻合。采用1572 nm KTP光参量振荡器作为拉曼激光器的腔内泵浦源有两个优势,一方面可以有效拓展拉曼变频的输出波长,另一方面可以基于光参量振荡器的脉冲窄化特性为后续多阶拉曼转换提供高强度的泵浦光。通过引入多阶级联拉曼变频的方案,为有效利用固体介质非常规低频移拉曼模式提供了新思路。
级联非线性频率变换 KGW晶体 多阶受激拉曼散射 1.7 μm cascade nonlinear frequency conversion KGW crystal multi-order stimulated Raman scattering 1.7 μm 
红外与激光工程
2022, 51(7): 20210507
作者单位
摘要
江苏师范大学物理与电子工程学院,江苏 徐州 221116

Tm3+离子3F4能级的粒子数捕获效应是影响2.3 μm掺铥激光器高效运转的重要因素。报道了基态吸收(GSA,3H63H4)和激发态吸收(ESA,3F43H4)双波长泵浦2.3 μm波段Tm∶YAP激光器。使用785 nm(GSA)和1470 nm(ESA)双波长泵浦方案能够精准减少3F4能级的粒子数,有效增加3H4能级粒子数布居。在双波长泵浦沿a轴切割的Tm∶YAP晶体中,使用透过率T=1.5%的输出镜,2274 nm和2383 nm双波长激光最大输出功率为2.28 W,相比于单波长泵浦方案提高了65.2%。使用T=2.8%输出镜,2383 nm激光的最大输出功率为942 mW,较单波长泵浦方案提高了84.3%。通过采用特殊镀膜的输出镜,进一步实现了2446 nm激光运转,最大输出功率为1.62 W,较单波长泵浦下的激光输出功率提高了48.6%。实验结果表明,GSA和ESA双波长泵浦方案为实现2.3 μm掺铥激光器获得更高的输出功率提供了一种有效技术手段。

激光器 2.3 μm掺铥激光器 基态吸收 激发态吸收 双波长泵浦 Tm∶YAP 
中国激光
2022, 49(1): 0101022
Author Affiliations
Abstract
School of Physics and Electronic Engineering, Jiangsu Normal University, Xuzhou 221116, China
The population trapping effect of the F34 level is an important factor limiting the power scaling of the 2.3 μm thulium (Tm) laser on the H34H35 transition. In this Letter, we demonstrate a novel scheme of ground state absorption (GSA) (H36H34) and excited state absorption (ESA) (F34H34) dual-wavelength pumped 2.3 μm Tm lasers. Introducing an ESA pumping process can accurately excite the Tm3+ ions accumulated in the F34 level to the H34 level, constructing a double populating mechanism for the upper laser level H34. A proof-of-principle experimental demonstration of the GSA (785 nm) and ESA (1470 nm) dual-wavelength pumped 2.3 μm Tm:LiYF4 (Tm:YLF) laser was realized. A maximum continuous-wave output power of 1.84 W at 2308 nm was achieved under 785 and 1470 nm dual-wavelength pumping, increased by 60% compared with the case of 785 nm single-wavelength pumping under the same resonator condition. Our work provides an efficient way to achieve higher output power from 2.3 μm Tm-doped lasers on the H34H35 transition.
2.3 μm thulium laser 3H4→3H5 transition dual-wavelength pumping 
Chinese Optics Letters
2021, 19(9): 091405
作者单位
摘要
1 江苏师范大学物理与电子工程学院, 江苏 徐州 221116
2 江苏师范大学江苏省先进激光技术与新兴产业协同创新中心, 江苏 徐州 221116
设计出一种基于级联非线性频率变换的634,644,655 nm多波长激光器。该复合变频过程由磷酸钛氧钾(KTP)和砷酸钛氧钾(KTA)晶体共同完成。首先由沿x轴切割的KTP晶体的光参量振荡将波长为1064 nm的激光变频为1572 nm,然后基于(θ=90°,φ=20.9°)切割KTA晶体完成1064 nm与1572 nm的和频过程,获得波长为634 nm的激光输出,进一步利用前述沿x轴切割KTP晶体的拉曼变频,将634 nm激光变频为644 nm的一阶拉曼光及655 nm的二阶拉曼光,实现634,644,655 nm多波长激光同时输出。该复合变频多波长激光器的最大平均输出功率为1.7 W,相应的脉冲宽度为19.3 ns,重复频率为6 kHz。
激光器 级联非线性光学频率变换 多波长激光器 KTiOPO4晶体 KTiOAsO4晶体 
中国激光
2019, 46(8): 0801003
作者单位
摘要
江苏师范大学物理与电子工程学院, 江苏 徐州 221116
具有低声子能量,高热导率的立方晶系倍半氧化物陶瓷是一种有潜力的铥掺杂激光材料,其常规3F4→3H6跃迁发射谱线可拓展至2.1 μm波段。综述了Tm∶Sc2O3、Tm∶Y2O3、Tm∶Lu2O3陶瓷的光谱参数和激光性能的研究进展,并指出复合结构及混晶型陶瓷是掺铥倍半氧化物陶瓷激光的未来发展方向。
激光器 掺铥固体激光器 2 μm波段 倍半氧化物 激光陶瓷 
激光与光电子学进展
2019, 56(9): 090001
黄海涛 1,2,*李敏 1金琳 1王辉 1[ ... ]沈德元 3
作者单位
摘要
1 江苏师范大学物理与电子工程学院, 江苏 徐州 221116
2 江苏省先进激光材料与器件重点实验室, 江苏 徐州 221116
3 复旦大学光科学与工程系, 上海 200433
受表面等离激元共振效应的影响, 金纳米棒饱和吸收体具有饱和吸收宽带可调、非线性响应时间快等特点, 且便于与各种激光谐振腔整合, 是一种有潜力的宽波段饱和吸收体材料。报道了一种基于金纳米棒饱和吸收体的1 μm波段被动调Q固体激光器。将金纳米棒溶液旋涂于输出镜上, 并将其作为可饱和吸收体构建到激光谐振腔中, 在LD端面抽运Nd∶YVO4激光器中实现了1064 nm被动调Q运转。在抽运功率为7.5 W时获得了平均输出功率为540 mW, 最小脉冲宽度为138 ns, 重复频率为602 kHz的脉冲激光输出。
激光器 金纳米棒 被动调Q 1 μm波段 
中国激光
2017, 44(7): 0703021
Author Affiliations
Abstract
1 Department of Optical Science and Engineering, Fudan University, Shanghai 200433, China
2 School of Physics and Electronic Engineering, Jiangsu Normal University, Xuzhou 221116, China
3 Jiangsu Collaborative Innovation Center of Advanced Laser Technology and Emerging Industry, Jiangsu Normal University, Xuzhou 221116, China
We report on a widely tunable, narrow linewidth operation of a Tm:YAG ceramic laser. A volume Bragg grating is used in the cavity as a folding mirror for wavelength selection. The wavelength is tuned from 1956.2 to 1995 nm, leading to a total tuning range of 38.7 nm. The linewidth is around 0.1 nm over the whole tuning range. A maximum output power of 1.51 W at 1990.5 nm is achieved at 37.8 W absorbed pump power. Different saturation behaviors are observed in the laser performances at different wavelengths.
140.3600 Lasers, tunable 140.3580 Lasers, solid-state 050.7330 Volume gratings 
Chinese Optics Letters
2015, 13(6): 061404
Author Affiliations
Abstract
1 Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
2 University of Chinese Academy of Sciences, Beijing 100049, China
3 Department of Optical Science and Engineering, Fudan University, Shanghai 200433, China
4 School of Physics and Electronic Engineering, Jiangsu Normal University, Xuzhou 221116, China
5 College of Physics and Microelectronic Science, Hunan University, Changsha 410082, China
Highly efficient and high-power operation of Raman fiber lasers in fixed-wavelength and wavelength-tunable cavity configurations based on a graded-index multimode fiber is reported. Fixed-wavelength and wavelength tunable operating regimes are achieved using volume Bragg gratings (VBGs) with center wavelengths of 1658 nm and 1750 nm, respectively. The fixed-wavelength laser yielded a maximum output power of 10.5 W at 1658.3 nm with a FWHM linewidth of ~0.1 nm for the launched pump power of 23.4 W, corresponding to a slope efficiency of 82.7% with respect to the launched pump power. The measured beam quality in the form of M2 factor is ~1.35, corresponding to the fundamental mode of the fiber. For the wavelength-tunable Raman fiber laser, a wavelength tuning range of 37 nm from 1638.5 to 1675.1 nm is obtained with a maximum output power of 3.6 W at 1658.5 nm for the launched pump power of 13.0 W.
Lasers and laser optics Lasers fiber Lasers Raman Nonlinear optics fibers 
Collection Of theses on high power laser and plasma physics
2014, 12(1): 6605
Author Affiliations
Abstract
1 Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
2 School of Physics and Electronic Engineering, Jiangsu Normal University, Xuzhou 221116, China
3 School of Information Science and Engineering, Department of Optical Science and Engineering, Fudan University, Shanghai 200433, China
We report high-power, dual-wavelength tunable operation of an Er:Yb co-doped fiber laser using two volume Bragg gratings arranged in parallel. The wavelength separation for the two operating wavelengths was continuously tuned from 0.3 to 29.2nm (0.04 to 3.7 THz) with a total output power of >13Wfor a wavelength splitting range of <20 nm. A maximum output power of 17.9W was obtained at a wavelength separation of 0.3nm for a launched pump power of 65.3W, which corresponds to a slope efficiency of 28.6% with respect to the launched pump power.
Collection Of theses on high power laser and plasma physics
2014, 12(1): 032702
Author Affiliations
Abstract
Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
A high-power and narrow-linewidth Er, Yb co-doped fiber laser is demonstrated by using two serially-paired volume Bragg gratings. A maximum output power of 19.4 W at 1545.3 nm with a full-width at half-maximum linewidth of <~38 pm is obtained for 65.3 W of launched pump power, corresponding to a slope efficiency of 30.1% with respect to launched pump power.
Er Yb fiber laser high-power narrow-linewidth volume Bragg grating 
Collection Of theses on high power laser and plasma physics
2014, 12(1): 88

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