Attosecond electron bunch compression scheme based on transverse gradient undulator
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摘要: 亚飞秒电子束在推动超快研究方面具有巨大潜力,包括超快电子衍射和自由电子激光。 然而传统压缩技术本质上受限于切片能散,难以产生亚飞秒电子束。本文提出基于横向梯度波荡器(TGU)的新压缩方案,利用TGU抑制切片能散,从而突破压缩极限。数值模拟表明,该方案可将电子束从50 fs压缩至1 fs以下。同时还讨论了电子枪中电场的相位和峰值电场抖动对束长压缩结果造成的影响,以及抑制该影响的手段。Abstract:
Background Sub-femtosecond electron beams offer enormous promise for furthering ultrafast research, including ultrafast electron diffraction and free-electron lasers. However, traditional compression techniques are essentially constrained by slice energy spread and cannot stably produce sub-femtosecond electron beams.Purpose This work proposes a unique compression strategy based on a Transverse Gradient Undulator (TGU). The slice energy spread is actively reduced by taking advantage of the link between transverse position and energy modulation in the TGU, hence breaking the compression limit.Methods Theoretical proof has been provided of the suppression effect of TGU on slice energy spread, with confirmation of the relevant parameters influencing this effect. A complete compression beamline has been designed, and numerical simulations conducted.Results Numerical simulations show that the proposed approach may compress the electron beam from 50 fs to less than 1 fs, with a compression factor over 52.09. Although phase jitter in the electron gun’s electric field affects the final compression pulse length, adjusting the modulation laser parameters of the TGU can effectively improve the compression results.Conclusions This study confirms that the TGU with flexible tunability and suppression of slice energy dispersion can be explored to be applied in ultrafast science research. -
Figure 1. Schematic of a TGU[25]
Table 1. The main parameters
Electric field
amplitudeLaunch
phaseOutput
energyBeam
chargeNumber of
electronsRadius
(rms)Initial pulse
duration (rms)175 MV/m 40° 3.793 MeV 20 fC 20000 50 μm 50 fs θ1 of D1,D2 LB1 of D1,D2 η of dogleg transverse gradient
α of TGUdimensionless parameter
K0 of TGUlaser
wavelengthlaser peak
power18° 0.1 m 0.05668 m55 m−1 1.5 1 mm 6.85 MW laser phase geometric strength of Q1 geometric strength of Q2 θ2 of D3 LB2 of D3 −32 ° 140 m−2 −49.1 m−2 5 ° 0.1 m -
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