Abstract

Electron transport in a nanowire exhibits a distinct behavior following the irradiation of intense laser pulse. Using particle-in-cell simulation, we observe a large-amplitude particle-driven wakefield excitation followed by electron acceleration in the solid density. Besides, we observed the quiver of the electrons across the nanowire under the action of the surrounding laser electric field facilitating deeper wakefield propagation in the nanowire with $2.5\ifmmode\times\else\texttimes\fi{}$ energy gain over a flat target. These results open insights into the laser-energy coupling with nanostructure targets and radiation sources, and motivate the wakefield acceleration in solid density plasma.

Highlights

  • The interaction of high-power lasers with nanostructure targets received a lot of attention lately due to their increased light-matter coupling efficiency [1,2,3,4]

  • A sinusoidal current inside the nanowire is generated soon after laser irradiation [see Fig. 1(a) and Supplemental Material (SM) Video 1 [25]]. This current has an amplitude of around | jx| = 0.4 MA/μm2, which corresponds to a current of 28 kA considering the area of the nanowire with diameter d

  • We have reported the wakefield generation in a solid density nanowire immediately following the interaction with an intense laser pulse

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Summary

Introduction

The interaction of high-power lasers with nanostructure targets received a lot of attention lately due to their increased light-matter coupling efficiency [1,2,3,4]. A laser pulse of relativistic intensity can heat a nanowire target to a much larger depth over a flat solid target [5]. Such an efficient laser energy absorption opens up various applications such as enhanced ion acceleration [6], attosecond bunch generation [7,8], enhanced x-ray [9,10,11,12,13], and gamma-ray generation [14], as well as efficient microfusion [5,15,16]. The laser energy absorption was mainly attributed to the vacuum heating through the laser electric field normal to the nanowire surfaces [18,19] and was utilized to optimize the electron acceleration [20]

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