基于改进的Frantz-Nodvik 方程的
Yb: KGW 再生放大器研究

doi:10.3969/j.issn.1007-5461.2022.04.012

量子电子学报 ›› 2022, Vol. 39 ›› Issue (4): 574-582.doi: 10.3969/j.issn.1007-5461.2022.04.012

基于改进的Frantz-Nodvik 方程的 Yb: KGW 再生放大器研究

康仁铸1;2, 吕仁冲1;2, 滕浩2;4, 朱江峰1, 魏志义1;2;3;4

( 1 西安电子科技大学物理与光电工程学院, 陕西西安710071; 2 中国科学院物理研究所, 北京凝聚态物理国家研究中心, 北京100190; 3 中国科学院大学物理科学学院, 北京100049; 4 松山湖材料实验室, 广东东莞523808 )

收稿日期:2021-01-15 修回日期:2021-02-06 出版日期:2022-07-28 发布日期:2022-07-28
通讯作者: E-mail: hteng@iphy.ac.cn; jfzhu@xidian.edu.cn E-mail:E-mail: hteng@iphy.ac.cn; jfzhu@xidian.edu.cn
作者简介:康仁铸( 1997 - ), 河南南阳人, 研究生, 主要从事超短脉冲激光放大方面的研究。E-mail: rzkang@stu.xidian.edu.cn
基金资助:
Supported by National Natural Science Foundation of China (国家自然科学基金, 12034020, 11774277), National Key R & D Program of China (国家重点研发计划, 2018YFB1107201), the Synergic Extreme Condition User Facility (综合极端条件实验装置)

Study on Yb: KGW regenerative amplifier based on improved Frantz-Nodvik equation

KANG Renzhu1;2, LYU Renchong1;2, TENG Hao2;4, ZHU Jiangfeng1, WEI Zhiyi1;2;3;4

( 1 School of Physics and Optoelectronic Engineering, Xidian University, Xi’an 710071, China; 2 Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China; 3 School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100049, China; 4 Songshan Lake Materials Laboratory, Dongguan 523808, China )

Received:2021-01-15 Revised:2021-02-06 Published:2022-07-28 Online:2022-07-28

摘要/Abstract

摘要： 超快激光再生放大过程具有复杂的动力学行为, 需要建立模型进行求解和迭代计算。基于改进的 Frantz-Nodvik 方程计算了Yb:KGW 晶体再生放大器的输出性质, 研究了泵浦强度、晶体长度和泵浦脉宽对放大器输出性能的影响, 同时对不同重复频率再生放大器的输出行为进行了分析。在此基础上设计了再生放大器, 得到了重复频率1 kHz、单脉冲能量1 mJ 的激光放大结果, 与理论分析结果符合得较好。该改进的Frantz-Nodvik 方程对于设计高重复频率、大能量且性能稳定的激光放大器具有参考价值。

关键词: 激光技术, Frantz-Nodvik 方程, 掺镱放大器, 再生放大

Abstract: The process of ultrafast laser regenerative amplification has complex dynamic behavior that requires to build a model for solution and iterative calculation. Based on the improved Frantz-Nodvik equation, the output properties of the Yb:KGW regenerative amplifier are calculated, the influences of pumping intensity, crystal length and pumping duration on the output performance of the amplifier are investigated, and the output behaviors of the regenerative amplifier with different repetition rates are also analyzed. Based on the theoretical analysis, a regenerative amplifier is constructed and the laser amplification results with pulse energy of 1 mJ at repetition rate of 1 kHz are realized, which are in good agreement with the theoretical analysis results. The improved Frantz-Nodvik equation gives an insight into the design of laser amplification which is scalable to high pulse energy with high stability at high repetition rate.

Key words: laser techniques, Frantz-Nodvik equation, ytterbium-doped amplifier, regenerative amplifier

中图分类号:

TN248.1

康仁铸, 吕仁冲, 滕浩, 朱江峰, 魏志义, . 基于改进的Frantz-Nodvik 方程的 Yb: KGW 再生放大器研究[J]. 量子电子学报, 2022, 39(4): 574-582.

KANG Renzhu, LYU Renchong, TENG Hao, ZHU Jiangfeng, WEI Zhiyi, . Study on Yb: KGW regenerative amplifier based on improved Frantz-Nodvik equation[J]. Chinese Journal of Quantum Electronics, 2022, 39(4): 574-582.

参考文献

[1]朱江峰，田文龙，高子叶等.二极管抽运全固态飞秒激光振荡器[J].中国激光, 2017, 44(09):1-10 [2]Tian W L, Peng Y N, Zhang Z Y, et al.Diode-pumped power scalable Kerr-lens mode-locked Yb:CYA laser[J].Photonics Research, 2018, 6(2):127-131 [3]Manjooran S, Major A.Diode-pumped 45fs Yb:CALGO laser oscillator with 17MW of peak power[J].Optics Letters, 2018, 43(10):2324-2327 [4]Kitajima S, Nakao H, Shirakawa A, et al.Kerr-lens mode-locked Yb3+-doped Lu3Al5O12 ceramic laser[J].Optics Letters, 2015, 41(19):4570-4573 [5]Ma J, Huang H, Ning K J, et al.Generation of 30-fs pulses from a diode-pumped graphene mode-locked Yb:CaYAlO4 laser[J].Optics Letters, 2015, 41(5):890-893 [6]赵智刚，丛振华，刘兆军.基于掺镱块材料的超短脉冲激光放大器综述[J].激光与光电子学进展, 2020, 57(07):70-83 [7] Sevillano P, Camy P, Doualan L, et al.130 fs - Multiwatt Yb:CaF2 regenerative amplifier pumped by a fiber laser[C]// Advanced Solid State Lasers, 2016. [8] Andriukaitis G, Kaksis E, Fl?ry T, et al.Cryogenically Cooled 30-mJ Yb:CaF2 Regenerative Amplifier[C]// Advanced Solid State Lasers, 2016. [9]Demirbas U, Cankaya H, Hua Y, et al.mJ,sub-ps pulses at up to 70 W average power from a cryogenic Yb:YLF regenerative amplifier[J].Optics Express, 2020, 28(2):2466-2479 [10]Caracciolo E, Kemnitzer M, Guandalini A, et al.W,217 fs solid-state Yb:CAlGdO4 regenerative amplifiers[J].Optics Letters, 2013, 38(20):4131-4133 [11]Caracciolo E, Pirzio F, Kemnitzer M, et al.W femtosecond Yb:Lu2O3 regenerative amplifier[J].Optics Letters, 2016, 41(15):3395-3398 [12]Rudenkov A, Kisel V, Yasukevich A, et al.Yb3+:CaYAlO4-based chirped pulse regenerative amplifier[J].Optics Letters, 2016, 41(10):2249-2252 [13]Rudenkov A, Kisel V, Matrosov V, et al.kHz 55W Yb3+: YVO4-based chirped-pulse regenerative amplifier[J].Optics Letters, 2015, 40(14):3352-3355 [14]Mackonis P, Rodin A M.Laser with 12 ps,20 mJ pulses at 100 Hz based on CPA with a low doping level Yb:YAG rods for seeding and pumping of OPCPA[J].Optics Express, 2020, 18(2):1261-1268 [15]Zhao Z G, Chen Q, Igarashi H, et al.Watt-level 193 nm source generation based on compact collinear cascaded sum frequency mixing configuration[J].Optics Express, 2018, 26(15):19435-19444 [16]Zapata L E, Reichert F, Hemmer M, et al.W average power,100 kHz repetition rate cryogenic Yb: YAG amplifier for OPCPA pumping[J].Optics letters, 2016, 41(3):492-495 [17]Wang N N, Wang X L, Zhang T, et al.W,985 fs Chirped Pulse Amplification System Based on Yb:YAG Rod Amplifier[J].IEEE Photonics Journal, 2019, 11(4):1-7 [18]Nubbemeyer T, Kaumanns M, Ueffing M, et al.kW,200mJ picosecond thin-disk laser system[J].Optics Letters, 2017, 42(7):1381-1384 [19]Kim G H, Yang J, Chizhov S A, et al.High average-power ultrafast CPA Yb:KYW laser system with dual-slab amplifier[J].Optics Express, 2012, 20(4):3434-3442 [20]Calendron A-L, Cankaya H, K?rtner F X.High-energy kHz Yb:KYW dual-crystal regenerative amplifier[J].Optics express, 2014, 22(20):24752-24762 [21]He H J, Yu J, Zhu W T, et al.A Yb:KGW dual-crystal regenerative amplifier[J].High Power Laser Science and Engineering, 2020, 8(35）.[J].High Power Laser Science and Engineering,2020,8（35):1-7 [22]Pouysegur J, Delaigue M, Zaouter Y, et al.Sub-100-fs Yb:CALGO nonlinear regenerative amplifier[J].Optics Letters, 2013, 38(23):5180-5183 [23]Yan D Y, Liu B W, Chu Y X, et al.Hybrid femtosecond laser system based on a Yb:KGW regenerative amplifier for NP polarization[J].Chinese Optics Letters, 2019, 17(4):75-78 [24]Frantz L M.and Nodvik J STheory of pulse propagation in a laser amplifier[J].Journal of Applied Physics, 1963, 34(8):2346-2349 [25]Grishin M, Gulbinas V, and Michailovas A.Dynamics of high repetition rate regenerative amplifiers[J].Optics express, 2007, 15(15):9434-9443 [26]Kroetz P, Ruehl A, Murari K, et al.Numerical study of spectral shaping in high energy Ho:YLF amplifiers[J].Optics Express, 2016, 24(9):9905-9921 [27]陆俊，刘征征，刘彦祺.等.突发运行模式下的飞秒碟片再生放大器[J].中国激光, 2017, 44(05):52-59 [28]Grafenstein L V, Bock M, and Griebner U.Bifurcation analysis in high repetition rate regenerative amplifiers[J].IEEE Journal of Selected Topics in Quantum Electronics, 2018, 24(5):1-13

基于改进的Frantz-Nodvik 方程的 Yb: KGW 再生放大器研究

Study on Yb: KGW regenerative amplifier based on improved Frantz-Nodvik equation

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