• High Power Laser Science and Engineering
  • Vol. 10, Issue 6, 06000e43 (2022)
Jingui Ma1, Xiaoping Ouyang2、*, Liangze Pan2, Peng Yuan1, Dongfang Zhang1, Jing Wang1, Guoqiang Xie1, Jianqiang Zhu2, and Liejia Qian1、3
Author Affiliations
  • 1Key Laboratory for Laser Plasmas (MOE), Collaborative Innovation Center of IFSA, School of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai, China
  • 2Joint Laboratory of High Power Laser and Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai, China
  • 3Tsung-Dao Lee Institute, Shanghai Jiao Tong University, Shanghai, China
  • show less
    DOI: 10.1017/hpl.2022.28 Cite this Article Set citation alerts
    Jingui Ma, Xiaoping Ouyang, Liangze Pan, Peng Yuan, Dongfang Zhang, Jing Wang, Guoqiang Xie, Jianqiang Zhu, Liejia Qian. Large temporal window and high-resolution single-shot cross-correlator with two separate measurement channels[J]. High Power Laser Science and Engineering, 2022, 10(6): 06000e43 Copy Citation Text show less

    Abstract

    In strong-field physics experiments with ultraintense lasers, a single-shot cross-correlator (SSCC) is essential for fast optimization of the pulse contrast and meaningful comparison with theory for each pulse shot. To simultaneously characterize an ultrashort pulse and its long pedestal, the SSCC device must have both a high resolution and a large temporal window. However, the resolution and window in all kinds of single-shot measurement contradict each other in principle. Here we propose and demonstrate a novel SSCC device with two separate measurement channels: channel-1 for the large-window pedestal measurement has a moderate resolution but a large window, while channel-2 for the ultrashort pulse measurement has a small window but a high resolution; this allows the accurate characterization of the pulse contrast in a single shot. A two-channel SSCC device with a 200-fs resolution and 114-ps window has been developed and tested for its application in ultraintense lasers at 800 nm.
    $$\begin{align}\Delta T = \frac{W}{c}\left({n}_{\mathrm{T}}\sin \alpha +{n}_{\mathrm{S}}\sin \beta \right),\end{align}$$ ((1))

    View in Article

    $$\begin{align}{\delta \tau}_{\mathrm{c}} = \frac{L}{c}\left({n}_{\mathrm{T}}\cos \alpha -{n}_{\mathrm{S}}\cos \beta \right).\end{align}$$ ((2))

    View in Article

    $$\begin{align}\delta \tau = \sqrt{\tau^2+{\delta \tau}_c^2+{\delta \tau}_d^2}.\end{align}$$ ((3))

    View in Article

    Jingui Ma, Xiaoping Ouyang, Liangze Pan, Peng Yuan, Dongfang Zhang, Jing Wang, Guoqiang Xie, Jianqiang Zhu, Liejia Qian. Large temporal window and high-resolution single-shot cross-correlator with two separate measurement channels[J]. High Power Laser Science and Engineering, 2022, 10(6): 06000e43
    Download Citation