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相对论飞秒激光等离子体Kα X射线发射的空间特性

Spatial characteristics of Kalpha x-ray emission from relativistic femtosecond laser plasmas.

作者信息

Reich Ch, Uschmann I, Ewald F, Düsterer S, Lübcke A, Schwoerer H, Sauerbrey R, Förster E, Gibbon P

机构信息

Institut für Optik und Quantenelektronik, Friedrich-Schiller-Universität Jena, Max-Wien-Platz 1, D-07743 Jena, Germany.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2003 Nov;68(5 Pt 2):056408. doi: 10.1103/PhysRevE.68.056408. Epub 2003 Nov 21.

Abstract

The spatial structure of the Kalpha emission from Ti targets irradiated with a high intensity femtosecond laser has been studied using a two-dimensional monochromatic imaging technique. For laser intensities I<5 x 10(17) W/cm(2), the observed spatial structure of the Kalpha emission can be explained by the scattering of the hot electrons inside the solid with the help of a hybrid particle-in-cell/Monte Carlo model. By contrast, at the maximum laser intensity I=7 x 10(18) W/cm(2) the half-width of the Kalpha emission was 70 microm compared to a laser-focus half-width of 3 microm. Moreover, the main Kalpha peak was surrounded by a halo of weak Kalpha emission with a diameter of 400 microm and the Kalpha intensity at the source center did not increase with increasing laser intensity. These three features point to the existence of strong self-induced fields, which redirect the hot electrons over the target surface.

摘要

利用二维单色成像技术研究了高强度飞秒激光辐照钛靶时Kα发射的空间结构。对于激光强度I<5×10¹⁷W/cm²的情况,借助混合粒子模拟/蒙特卡罗模型,热电子在固体内部的散射可以解释观测到的Kα发射的空间结构。相比之下,在最大激光强度I = 7×10¹⁸W/cm²时,Kα发射的半高宽为70微米,而激光聚焦半高宽为3微米。此外,主要的Kα峰被直径为400微米的弱Kα发射晕包围,并且源中心处的Kα强度并未随激光强度的增加而增加。这三个特征表明存在强自感应场,该场会使热电子在靶表面重新定向。

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