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Main > High Power Laser Science and Engineering >  Volume 7 >  Issue 3 >  Page 03000e54 > Article
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    • Received: Mar. 10, 2019

    Accepted: Jun. 21, 2019

    Posted: Aug. 26, 2019

    Published Online: Aug. 26, 2019

    The Author Email: Colin N. Danson (c.danson@imperial.ac.uk)

    DOI: 10.1017/hpl.2019.36

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    Colin N. Danson, Constantin Haefner, Jake Bromage, Thomas Butcher, Jean-Christophe F. Chanteloup, Enam A. Chowdhury, Almantas Galvanauskas, Leonida A. Gizzi, Joachim Hein, David I. Hillier, Nicholas W. Hopps, Yoshiaki Kato, Efim A. Khazanov, Ryosuke Kodama, Georg Korn, Ruxin Li, Yutong Li, Jens Limpert, Jingui Ma, Chang Hee Nam, David Neely, Dimitrios Papadopoulos, Rory R. Penman, Liejia Qian, Jorge J. Rocca, Andrey A. Shaykin, Craig W. Siders, Christopher Spindloe, Sándor Szatmári, Raoul M. G. M. Trines, Jianqiang Zhu, Ping Zhu, Jonathan D. Zuegel. Petawatt and exawatt class lasers worldwide[J]. High Power Laser Science and Engineering, 2019, 7(3): 03000e54

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$$\begin{eqnarray}U_{p}=\frac{e^{2}}{8\unicode[STIX]{x1D70B}c^{3}\unicode[STIX]{x1D700}_{0}m_{e}}I\unicode[STIX]{x1D706}^{2},\end{eqnarray}$$(1)

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$$\begin{eqnarray}n_{e}=\frac{4\unicode[STIX]{x1D70B}c^{2}\unicode[STIX]{x1D700}_{0}m_{e}}{e^{2}}\unicode[STIX]{x1D706}^{-2},\end{eqnarray}$$(2)

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$$\begin{eqnarray}n=\sqrt[]{1-\frac{\unicode[STIX]{x1D714}_{p}^{2}}{\unicode[STIX]{x1D714}_{\text{probe}}^{2}}}\end{eqnarray}$$(3)

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