Abstract

The complex physics of the interaction between short pulse high intensity lasers and solids is so far hardly accessible by experiments. As a result of missing experimental capabilities to probe the complex electron dynamics and competing instabilities, this impedes the development of compact laser-based next generation secondary radiation sources, e.g. for tumor therapy [Bulanov2002,ledingham2007], laboratory-astrophysics [Remington1999,Bulanov2015], and fusion [Tabak2014]. At present, the fundamental plasma dynamics that occur at the nanometer and femtosecond scales during the laser-solid interaction can only be elucidated by simulations. Here we show experimentally that small angle X-ray scattering of femtosecond X-ray free-electron laser pulses facilitates new capabilities for direct in-situ characterization of intense short-pulse laser plasma interaction at solid density that allows simultaneous nanometer spatial and femtosecond temporal resolution, directly verifying numerical simulations of the electron density dynamics during the short pulse high intensity laser irradiation of a solid density target. For laser-driven grating targets, we measure the solid density plasma expansion and observe the generation of a transient grating structure in front of the pre-inscribed grating, due to plasma expansion, which is an hitherto unknown effect. We expect that our results will pave the way for novel time-resolved studies, guiding the development of future laser-driven particle and photon sources from solid targets.

Highlights

  • The density maxima are interleaved, forming a double frequency grating in x-ray free-electron laser projection for a short time, which is a hitherto unknown effect

  • SACLA in the near future [47], here we report on a scattering experiment with the currently most intense optical pump laser available at an x-ray freeelectron laser (XFEL), the short-pulse highintensity (HI) laser at the Matter in Extreme Conditions (MEC) end station of Linac Coherent Light Source (LCLS) at SLAC [48,49]

  • The scattering signal covers the whole field of view of the detector, with decreasing intensity at larger scattering vector values q ≡ ð2π=λXÞ2 sinðΘ=2Þ

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Summary

Introduction

The solid-density plasmas created in the interaction of an ultrashort, ultrahigh-intensity (UHI) laser pulse with a solid target are a source of femtosecond, high-charge electron [6] and ion bunches [7,8,9,10], extreme ultraviolet (XUV) radiation [11,12,13], and neutrons [14], making them promising candidates for future particle accelerators or radiation. The fundamental property of such ultraintense lasers is the acceleration of plasma electrons to relativistic energies within a single laser period, i.e., less than a few femtoseconds in the case of optical or nearinfrared UHI lasers.

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