V Grafenstein K, Foerster F M, Haberstroh F, Campbell D, Irshad F, Salgado F C, Schilling G, Travac E, Weiße N, Zepf M, Döpp A, Karsch S
Ludwig-Maximilians-Universität München, Centre for Advanced Laser Applications, 85748, Garching, Germany.
Department of Physics, University of Strathclyde, Glasgow, G4 0NG, UK.
Sci Rep. 2023 Jul 19;13(1):11680. doi: 10.1038/s41598-023-38805-3.
In recent years, significant progress has been made in laser wakefield acceleration (LWFA), both regarding the increase in electron energy, charge and stability as well as the reduction of bandwidth of electron bunches. Simultaneous optimization of these parameters is, however, still the subject of an ongoing effort in the community to reach sufficient beam quality for next generation's compact accelerators. In this report, we show the design of slit-shaped gas nozzles providing centimeter-long supersonic gas jets that can be used as targets for the acceleration of electrons to the GeV regime. In LWFA experiments at the Centre for Advanced Laser Applications, we show that electron bunches are accelerated to [Formula: see text] using these nozzles. The electron bunches were injected into the laser wakefield via a laser-machined density down-ramp using hydrodynamic optical-field-ionization and subsequent plasma expansion on a ns-timescale. This injection method provides highly controllable quasi-monoenergetic electron beams with high charge around [Formula: see text], low divergence of [Formula: see text], and a relatively small energy spread of around [Formula: see text] at [Formula: see text]. In contrast to capillaries and gas cells, the scheme allows full plasma access for injection, probing or guiding in order to further improve the energy and quality of LWFA beams.
近年来,激光尾场加速(LWFA)取得了重大进展,在电子能量、电荷量和稳定性的提高以及电子束团带宽的降低方面均有成效。然而,同时优化这些参数仍是该领域持续努力的方向,目的是为下一代紧凑型加速器实现足够的束流质量。在本报告中,我们展示了狭缝形气体喷嘴的设计,该喷嘴可产生厘米级长的超音速气体射流,可用作将电子加速至GeV量级的靶材。在先进激光应用中心的LWFA实验中,我们展示了使用这些喷嘴可将电子束团加速至[公式:见原文]。电子束团通过激光加工的密度下降斜坡,利用流体动力学光场电离以及随后纳秒级的等离子体膨胀注入激光尾场。这种注入方法可提供高度可控的准单能电子束,电荷量约为[公式:见原文],发散角为[公式:见原文],在[公式:见原文]时能量分散相对较小,约为[公式:见原文]。与毛细管和气体池不同,该方案允许完全进入等离子体进行注入、探测或引导,以进一步提高LWFA束流的能量和质量。