Abstract

Recently, the short-pulse intense laser has become a common tool for studying the relativistic plasma with tremendous physical parameters. And the laser-driven magnetic reconnection is one of the hot topics and has received much attention. The laser-driven magnetic reconnection experiments are usually conducted by closely focusing two laser beams on a planar coil target. However, it is always hard to distinguish the physical property of magnetic reconnection from the complex background of laser-produced plasma. In this paper, we present the particle-in-cell simulation results of magnetic reconnection driven by two short-pulse lasers as well as a single laser pulse irradiating the solid planar target, and discuss the correlation between the potential distribution behind the target and the magnetic reconnection. When a single laser is used, the potential behind the target shows a double-peak distribution, which is in agreement with recent experimental results. When two lasers irradiate the target, the potential behind the target shows a three-peak distribution. The accumulated spatial distribution of plasma ions with fixed energy (4.5 and 6 MeV) at 3 μm behind the target shows several peaks, which is in agreement with the potential distribution when either a single laser or two lasers are used. In addition, after the laser pulse terminates, in the two-laser case there is extremely strong effect on the topological structure of the electric field compared with in the singlelaser case. When the magnetic reconnection happens (which can be identified through the reconnection electric field and the electron energy spectrum), the amplitude of the <i>x</i> component of the electric field has different evolution characteristics from the single laser case. The line outs of the <i>y</i> component of the electric field in two cases also have completely different shapes. In summary, the simulation results reveal that the potential distribution behind the target can directly affect the spatial distribution of the accelerated ions. This could be possibly used to identify the short pulse laser-driven magnetic reconnection in experiment.

Highlights

  • Sheath electric field Ex curves over time at (a) the front target and (b) the rear target

  • 图 3 (a) 单束激光 (蓝色) 和两束激光 (橙色) 对时间取平均后得到的靶后电势分布; (b) 磁重联过程的示意图 Fig. 3. (a) Electric potential distribution averaged over certain time at the target back obtained from the data of single laser and two lasers respectively; (b) the illustration of magnetic reconnection process

  • 这个结论可以通过超短超强激光驱动磁 重联的实验来验证, 记录实验中靶后 RCF 的成像 结果, 成像结果理论上会存在两个并列的环状结 构

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Summary

Introduction

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