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超快超强激光系统中消色差透镜组装调误差引入的“空-时”耦合畸变分析

许浩天 王逍 李伟 孙斌 王冀敏 卫鹏宇 母杰 李纲 左言磊

许浩天, 王逍, 李伟, 等. 超快超强激光系统中消色差透镜组装调误差引入的“空-时”耦合畸变分析[J]. 强激光与粒子束. doi: 10.11884/HPLPB202537.250002
引用本文: 许浩天, 王逍, 李伟, 等. 超快超强激光系统中消色差透镜组装调误差引入的“空-时”耦合畸变分析[J]. 强激光与粒子束. doi: 10.11884/HPLPB202537.250002
Xu Haotian, Wang Xiao, Li Wei, et al. Analysis of spatio-temporal coupling aberrations introduced by achromatic lens assembly tuning errors in ultrafast and ultra intense laser systems[J]. High Power Laser and Particle Beams. doi: 10.11884/HPLPB202537.250002
Citation: Xu Haotian, Wang Xiao, Li Wei, et al. Analysis of spatio-temporal coupling aberrations introduced by achromatic lens assembly tuning errors in ultrafast and ultra intense laser systems[J]. High Power Laser and Particle Beams. doi: 10.11884/HPLPB202537.250002

超快超强激光系统中消色差透镜组装调误差引入的“空-时”耦合畸变分析

doi: 10.11884/HPLPB202537.250002
基金项目: 国家重点研发计划项目(2022YFB3606305);国防基础科研计划项目(JCKYS2022212804)
详细信息
    作者简介:

    许浩天,xht0032@mail.ustc.edu.cn

    通讯作者:

    王 逍,wangxiaocn@263.net

  • 中图分类号: O438.2

Analysis of spatio-temporal coupling aberrations introduced by achromatic lens assembly tuning errors in ultrafast and ultra intense laser systems

  • 摘要: 在超快超强激光系统中,通常会使用消色差透镜组代替普通的扩束透镜,以消除后者自身存在的色差导致的脉冲激光的“空-时”耦合(STCs)畸变。然而,消色差透镜组对装调精度要求非常高,装调误差的存在会引入新的“空-时”耦合畸变,使脉冲激光的远场功率密度下降,达不到预期的消色差效果。针对工程实践中常见的几种消色差透镜组装调误差,详细分析了其引入的“空-时”耦合畸变,并且根据其对远场聚焦功率密度的影响给出了不同种类装调误差的容许范围。分析过程采用了宽光谱脉冲激光传输演化模型及厚透镜等效位相屏演化模型,该模型可以精确地表征激光近远场的“空-时”特性。
  • 图  1  空间滤波器示意图

    Figure  1.  Schematic diagram of spatial filter

    图  2  消色差透镜示意图

    Figure  2.  Schematic diagram of achromatic lens

    图  3  宽光谱脉冲激光传输演化模型

    Figure  3.  Computational modeling of broad-spectrum pulsed laser transmission

    图  4  厚透镜的等效位相屏演化模型

    Figure  4.  Computational model of equivalent phase screen for thick lenses

    图  5  SILEX-II激光装置中的空间滤波器示意图

    Figure  5.  Schematic diagram of the spatial filter in the SILEX-II laser unit

    图  6  各波长的近场波前

    Figure  6.  Near-field wave fronts for each wavelength

    图  7  空间滤波器输出后的近场分布

    Figure  7.  Near-field distribution after spatial filter output

    图  8  “空-时”场分布

    Figure  8.  Spatio-time field distribution

    图  9  光强的空间或时间分布

    Figure  9.  Spatial or temporal field distribution

    图  10  消色差透镜组几种典型的装调误差

    Figure  10.  Typical mounting errors for achromatic lens sets

    图  11  存在装调误差时激光脉冲的“空-时”场分布

    Figure  11.  Spatio-temporal field distribution of laser pulses in the presence of mounting errors

    图  12  远场峰值功率密度与不同误差的关系

    Figure  12.  Far-field peak power density versus different errors

    表  1  透镜组参数(使用普通透镜组)

    Table  1.   Parameters of lens set (using common lens set)

    lens set lens $ R_1/{\mathrm{mm}} $ $ R_2/{\mathrm{mm}} $ $ {d}_{{\mathrm{c}}}/{\mathrm{mm}} $ $ f/{\mathrm{mm}} $ material
    SF1 L1 153.238 $ \mathrm{\infty } $ 10 300 K9
    L2 $ \mathrm{\infty } $ −153.238 10 300 K9
    SF2 L1 179.200 1026.250 20 300 K9
    L2 887.370 5617.620 20 1500 K9
    SF3 L1 156.110 376.212 15 500 K9
    L2 1066.410 6644.320 40 1800 K9
    SF4 L1 1365.150 8490.090 30 2300 K9
    L2 4090.740 25782.400 30 6900 K9
    下载: 导出CSV

    表  2  透镜组参数(使用消色差透镜)

    Table  2.   Parameters of lens set (using achromatic lenses)

    lens set lens $ R_1/{\mathrm{mm}} $ $ R_2/{\mathrm{mm}} $ $ {d}_{{\mathrm{c}}}/{\mathrm{mm}} $ $ f/{\mathrm{mm}} $ material
    SF1 L1 153.238 $ \mathrm{\infty } $ 10 300 K9
    L2 $ \mathrm{\infty } $ −153.238 10 300 K9
    SF2 L1 179.200 1026.250 20 300 K9
    L2 887.370 5617.620 20 1500 K9
    SF3 L1 156.110 376.212 15 500 K9
    L2 1066.410 6644.320 40 1800 K9
    SF4 L1-1 275.800 −349.348 55 2100 K9
    L1-2 −349.348 844.100 20 ZF7
    L2 4090.740 25782.400 30 6900 K9
    下载: 导出CSV
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  • 收稿日期:  2025-01-03
  • 修回日期:  2025-05-17
  • 录用日期:  2025-05-26
  • 网络出版日期:  2025-05-27

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