• Acta Physica Sinica
  • Vol. 68, Issue 21, 214204-1 (2019)
Yu-Jiao Jiang1, Yi-Tan Gao2、3, Pei Huang3、4, Kun Zhao2、*, Si-Yuan Xu1, Jiang-Feng Zhu1, Shao-Bo Fang2, Hao Teng2, Xun Hou4, and Zhi-Yi Wei2、3、*
Author Affiliations
  • 1School of Physics and Optoelectronic Engineering, Xidian University, Xi’an 710071, China
  • 2Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
  • 3University of Chinese Academy of Sciences, Beijing 100049, China
  • 4Xi’an Institute of Optics and Precision Mechanics, Chinese Academy of Sciences, Xi’an 710119, China
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    DOI: 10.7498/aps.68.20191164 Cite this Article
    Yu-Jiao Jiang, Yi-Tan Gao, Pei Huang, Kun Zhao, Si-Yuan Xu, Jiang-Feng Zhu, Shao-Bo Fang, Hao Teng, Xun Hou, Zhi-Yi Wei. Phase control and stabilization in attosecond beamline with fast Fourier transform[J]. Acta Physica Sinica, 2019, 68(21): 214204-1 Copy Citation Text show less
    Sketch of the pump-probe setup (m1−m15, flat mirror; f1, flat-concave lens; f2, f3, convex lens).抽运探测实验示意图 (m1−m15, 平面高反镜; f1, 平凹透镜; f2, f3, 凸透镜)
    Fig. 1. Sketch of the pump-probe setup (m1−m15, flat mirror; f1, flat-concave lens; f2, f3, convex lens).抽运探测实验示意图 (m1−m15, 平面高反镜; f1, 平凹透镜; f2, f3, 凸透镜)
    Arm length stabilization of a Mach-Zehnder interferometer (M1, concave lens; M2, convex lens; M3−M10, plane mirrors; P, polarizer;, half wave plate; FL, focusing lens; CW, continuous wave).用532 nm连续激光干涉锁定光路示意图(M1, 凹透镜; M2, 凸透镜; BS, 分束片; M3−M10, 平面银镜; P, 偏振片;, 半波片; FL, 凸透镜; CW, 连续)
    Fig. 2. Arm length stabilization of a Mach-Zehnder interferometer (M1, concave lens; M2, convex lens; M3−M10, plane mirrors; P, polarizer; , half wave plate; FL, focusing lens; CW, continuous wave). 用532 nm连续激光干涉锁定光路示意图(M1, 凹透镜; M2, 凸透镜; BS, 分束片; M3−M10, 平面银镜; P, 偏振片; , 半波片; FL, 凸透镜; CW, 连续)
    Interferometer locking stability over 12 hours. Inset is the relative phase drift when armlength is not locked.用532 nm连续激光干涉锁定12 h的稳定性, 其中均方差为14.6 mrad, 插图为未锁定下的相对相位漂移
    Fig. 3. Interferometer locking stability over 12 hours. Inset is the relative phase drift when armlength is not locked.用532 nm连续激光干涉锁定12 h的稳定性, 其中均方差为14.6 mrad, 插图为未锁定下的相对相位漂移
    Actual electric field of a few cycle laser pulse under different CEP values, which affect the electric field significantly.在同一脉冲包络下不同CEP值所对应的实际电场(CEP对少周期脉冲电场实际形状影响显著)
    Fig. 4. Actual electric field of a few cycle laser pulse under different CEP values, which affect the electric field significantly.在同一脉冲包络下不同CEP值所对应的实际电场(CEP对少周期脉冲电场实际形状影响显著)
    f-2f setup diagram, where collinear design is applied to avoid delay variation.f-2f装置光路图(采用共线设计以避免延时变化)
    Fig. 5. f-2f setup diagram, where collinear design is applied to avoid delay variation. f-2f装置光路图(采用共线设计以避免延时变化)
    CEP offset over 20 minutes when CEP is locked using f-2f.f-2f锁定CEP20分钟的效果(均方差为227 mrad)
    Fig. 6. CEP offset over 20 minutes when CEP is locked using f-2f. f-2f锁定CEP20分钟的效果(均方差为227 mrad)
    Yu-Jiao Jiang, Yi-Tan Gao, Pei Huang, Kun Zhao, Si-Yuan Xu, Jiang-Feng Zhu, Shao-Bo Fang, Hao Teng, Xun Hou, Zhi-Yi Wei. Phase control and stabilization in attosecond beamline with fast Fourier transform[J]. Acta Physica Sinica, 2019, 68(21): 214204-1
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