Acta Physica Sinica, Volume. 68, Issue 21, 214204-1(2019)
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)
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)
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
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)
Fig. 5.
Fig. 6. CEP offset over 20 minutes when CEP is locked using
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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.
Received: Jul. 29, 2019
Accepted: --
Published Online: Sep. 17, 2020
The Author Email: Wei Zhi-Yi (zywei@iphy.ac.cn)