First high peak and average power single-pass THz FEL based on high brightness photoinjector

M. Krasilnikov, Z. Aboulbanine, G. Adhikari, N. Aftab, A. Asoyan, P. Boonpornprasert, H. Davtyan, G. Georgiev, J. Good, A. Grebinyk, M. Gross, A. Hoffmann, E. Kongmon, X. -K. Li, A. Lueangaramwong, D. Melkumyan, S. Mohanty, R. Niemczyk, A. Oppelt, H. Qian, C. Richard, F. Stephan, G. Vashchenko, T. Weilbach, X. Zhang, M. Tischer, E. Schneidmiller, P. Vagin, M. Yurkov, E. Zapolnova, W. Hillert, J. Rossbach A. Brachmann, N. Holtkamp, H. -D. Nuhn
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Abstract

Advanced experiments using THz pump and X-ray probe pulses at modern free-electron lasers (FELs) like the European X-ray FEL require a frequency-tunable, high-power, narrow-band THz source maintaining the repetition rate and pulse structure of the X-ray pulses. This paper reports the first results from a THz source, that is based on a single-pass high-gain THz FEL operating with a central wavelength of 100 micrometers. The THz FEL prototype is currently in operation at the Photo Injector Test facility at DESY in Zeuthen (PITZ) and uses the same type of electron source as the European XFEL photo injector. A self-amplified spontaneous emission (SASE) FEL was envisioned as the main mechanism for generating the THz pulses. Although the THz FEL at PITZ is supposed to use the same mechanism as at X-ray facilities, it cannot be considered as a simple scaling of the radiation wavelength because there is a large difference in the number of electrons per radiation wavelength, which is five orders of magnitude higher for the THz case. The bunching factor arising from the electron beam current profile contributes strongly to the initial spontaneous emission starting the FEL process. Proof-of-principle experiments were done at PITZ using an LCLS-I undulator to generate the first high-power, high-repetition-rate single-pass THz FEL radiation. Electron bunches with a beam energy of ~17 MeV and a bunch charge of up to several nC are used to generate THz pulses with a pulse energy of several tens of microjoules. For example, for an electron beam with a charge of ~2.4 nC, more than 100 microjoules were generated at a central wavelength of 100 micrometers. The narrowband spectrum was also demonstrated by spectral measurements. These proof-of-principle experiments pave the way for a tunable, high-repetition-rate THz source providing pulses with energies in the millijoule range.
首个基于高亮度光注入器的高峰值和平均功率单通太赫兹 FEL
在现代自由电子激光器(FEL)(如欧洲 X 射线 FEL)上使用太赫兹泵浦脉冲和 X 射线探针脉冲进行高级实验,需要频率可调、高功率、窄带太赫兹源,以保持 X 射线脉冲的脉冲频率和脉冲结构。本文报告了基于中心波长为 100 微米的单通道高增益 THzFEL 的 THz 源的首批结果。太赫兹 FEL 原型目前正在宙申(PITZ)DESY 的光注入器测试设备上运行,使用与欧洲 XFEL 光注入器相同类型的电子源。自放大自发辐射(SASE)FEL 是产生太赫兹脉冲的主要机制。尽管 PITZ 的太赫兹 FEL 应该使用与 X 射线设施相同的机制,但不能将其视为辐射波长的简单缩放,因为每个辐射波长的电子数量差异很大,太赫兹情况下要高出五个数量级。PITZ使用LCLS-I型减压器进行了原理验证实验,产生了首个高功率、高重复率的单通道太赫兹FEL辐射。束流能量约为 17 MeV、束流电荷高达几 nC 的电子束被用来产生脉冲能量为几十微焦耳的太赫兹脉冲。例如,对于电荷量约为 2.4nC 的电子束,在中心波长为 100 厘米时可产生超过 100 微焦的脉冲能量。窄带光谱也通过光谱测量得到了证明。这些原理验证实验为可调谐、高重复率太赫兹源提供毫焦耳范围内的脉冲能量铺平了道路。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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