• High Power Laser Science and Engineering
  • Vol. 11, Issue 3, 03000e36 (2023)
Kangnan Jiang1、2, Ke Feng1、*, Hao Wang1, Xiaojun Yang1, Peile Bai1, Yi Xu1, Yuxin Leng1, Wentao Wang1、*, and Ruxin Li1、2、*
Author Affiliations
  • 1State Key Laboratory of High Field Laser Physics and CAS Center for Excellence in Ultra-intense Laser Science, Shanghai Institute of Optics and Fine Mechanics (SIOM), Chinese Academy of Sciences (CAS), Shanghai, China
  • 2School of Physical Science and Technology, ShanghaiTech University, Shanghai, China
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    DOI: 10.1017/hpl.2023.9 Cite this Article Set citation alerts
    Kangnan Jiang, Ke Feng, Hao Wang, Xiaojun Yang, Peile Bai, Yi Xu, Yuxin Leng, Wentao Wang, Ruxin Li, "Measurement of electron beam transverse slice emittance using a focused beamline," High Power Laser Sci. Eng. 11, 03000e36 (2023) Copy Citation Text show less

    Abstract

    A single-shot measurement of electron emittance was experimentally accomplished using a focused transfer line with a dipole. The betatron phase of electrons based on laser wakefield acceleration (LWFA) is energy dependent owing to the coupling of the longitudinal acceleration field and the transverse focusing (defocusing) field in the bubble. The phase space presents slice information after phase compensation relative to the center energy. Fitting the transverse size of the electron beam at different energy slices in the energy spectrum measured 0.27 mm mrad in the experiment. The diagnosis of slice emittance facilitates local electron quality manipulation, which is important for the development of LWFA-based free electron lasers. The quasi-3D particle-in-cell simulations matched the experimental results and analysis well.
    $$\begin{align}\phi = \frac{\sqrt{2}{k}_{\mathrm{p}}}{\gamma^{\prime }}\left(\sqrt{\gamma (0)+{\gamma}^{\prime }l}-\sqrt{\gamma (0)}\right),\end{align}$$ ((1))

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    $$\begin{align}\Delta \phi (l) = {\phi}_{\mathrm{H}}(l)-{\phi}_{\mathrm{L}}(l)+\Delta {\phi}_0,\end{align}$$ ((2))

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    $$\begin{align}\left(\begin{array}{@{}c@{}}r\\ {}{r}^{\prime}\end{array}\right) {=} \left(\begin{array}{@{}cc@{}}{M}_{11}& {M}_{12}\\ {}{M}_{21}& {M}_{22}\end{array}\right)\!\left(\begin{array}{@{}c@{\ }c@{}}\cos \left(\Delta \phi \right)& \sin \left(\Delta \phi \right)/{k}_{\beta}\\ {}-{k}_{\beta}\cdot \sin \left(\Delta \phi \right)& \cos \left(\Delta \phi \right)\end{array}\right)\!\left(\begin{array}{@{}c@{}}{r}_0\\ {}{r}_0^{\prime}\end{array}\right)\!,\end{align}$$ ((3))

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    $$\begin{align}{\sigma}_y^2 = {R}_{11}^2\varepsilon {\beta}_0-2{R}_{11}{R}_{12}\varepsilon {\alpha}_0+{R}_{12}^2\varepsilon {\gamma}_0,\end{align}$$ ((4))

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    Kangnan Jiang, Ke Feng, Hao Wang, Xiaojun Yang, Peile Bai, Yi Xu, Yuxin Leng, Wentao Wang, Ruxin Li, "Measurement of electron beam transverse slice emittance using a focused beamline," High Power Laser Sci. Eng. 11, 03000e36 (2023)
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