赵智刚 1,2玄洪文 3,**王景冲 2丛振华 1,2[ ... ]刘兆军 1,2,*
作者单位
摘要
1 山东大学信息科学与工程学院, 山东省激光技术与应用重点实验室, 山东 青岛 266237
2 山东大学激光与红外系统集成技术教育部重点实验室, 山东 青岛 266237
3 广东大湾区空天信息研究院, 广东 广州 510700
4 东京大学物性研究所, 日本 千叶 277-8581

综述了真空紫外193 nm波段固体激光光源的发展情况,具体包括所涉及到的主要非线性晶体[偏硼酸钡(BBO)晶体、三硼酸锂(LBO)晶体、六硼酸铯锂(CLBO)晶体、氟代硼铍酸钾(KBBF)晶体等]的各类特性及其对比分析、近几十年来193 nm波段连续固体激光和脉冲固体激光的发展脉络、用于产生193 nm固体激光的各种基频光源组合,并对它们的优劣势进行了分类分析和对比。对影响非线性晶体紫外透过率和紫外激光输出功率的双光子吸收效应进行了描述,并对深紫外激光器中的激光诱导污染效应进行了描述,指出几类常用的避免或者缓解该效应的方法。最后对实现超高重复频率准连续真空紫外激光的难度和应当解决的问题进行了探讨。

深紫外 固体激光 真空紫外 非线性晶体 双光子吸收 激光诱导污染 
光学学报
2022, 42(11): 1134010
Author Affiliations
Abstract
1 The Institute for Solid State Physics, The University of Tokyo, Kashiwa, Chiba 277-8581, Japan
2 Current affiliation: School of Information Science and Engineering, Shandong University, Qingdao 266237, China
A monolithic lens-window-prism (LWP) device, made of lithium fluoride (LiF) or magnesium fluoride (MgF2), was proposed. When either of the devices was fixed onto one end of a gas cell filled with Xe, it becomes a “wedge-crystal”-like device and was used to convert a 1 MHz femtosecond 347 nm laser to its third harmonic radiation at 10.7 eV. This led to an improved beam profile and a more compact and less lossy configuration. A stable output power of ~11 μW was demonstrated for 2 h using LiF-LWP. In addition, MgF2-LWP was also verified for its practicability at 10.7 eV.
140.7240 UV, EUV, and X-ray lasers 190.2620 Harmonic generation and mixing 320.7090 Ultrafast lasers 
Chinese Optics Letters
2019, 17(5): 051406
Author Affiliations
Abstract
1 The Institute for Solid State Physics, The University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8581, Japan
2 Department of Physics, Graduate School of Science, The University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-0033, Japan
Efficient high harmonics generation (HHG) was demonstrated at 10 MHz repetition rate with an external femtosecond enhancement cavity, seeded by a ${\sim}70~\text{fs}$ post-compressed 10 MHz fiber chirped pulse amplifier (FCPA) laser. Operation lasting over 30 min with 0.1 mW outcoupled power at 149 nm was demonstrated. It was found that shorter pulse was beneficial for alleviating the nonlinear plasma effect and improving the efficiency of HHG. Low finesse cavity can relax the plasma nonlinearity clamped intra-cavity power and improve the cavity-locking stability. The pulse duration is expected to be below 100 fs for both 1040 nm and 149 nm outputs, making it ideal for applications such as time-resolved photoemission spectroscopy.
enhancement cavity high harmonics generation ultrafast fiber lasers. 
High Power Laser Science and Engineering
2018, 6(2): 02000e19
Author Affiliations
Abstract
1 Institue for Solid State Physics, University of Tokyo, Kashiwanoha, Kashiwa, Chiba 277-8581, Japan
2 HiLASE Centre, Institute of Physics ASCR, v.v.i., Za Radnici 828, 25241 Dolni Brezany, Czech Republic
The group-delay dispersion of an optical fiber was measured with the time-of-flight method, using fingerprint-like characteristic spectra from a mode-locked fiber laser source. To determine the group-delay dispersion up to the fourth order, least-squares fitting was applied to the overall time waveform mapped on the time axis for the fingerprint- spectral broadband pulses through a long optical fiber. The analysis of all 4003 data points reduced statistical uncertainty, and provided second-, third-, and fourth-order dispersion with uncertainties of 0.02%, 0.4%, and 4%, respectively.
Fiber characterization Fiber characterization Dispersion Dispersion Lasers Lasers fiber fiber Probability theory Probability theory stochastic processes stochastic processes and statistics and statistics 
Photonics Research
2016, 4(1): 01000013

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