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通过失谐X射线自由电子激光波荡器调整阿秒脉冲的放大

Tailoring the amplification of attosecond pulse through detuned X-ray FEL undulator.

作者信息

Kumar Sandeep, Kang Heung-Sik, Kim Dong Eon

出版信息

Opt Express. 2015 Feb 9;23(3):2808-18. doi: 10.1364/OE.23.002808.

DOI:10.1364/OE.23.002808
PMID:25836141
Abstract

We demonstrate that the amplification of attosecond pulse in X-ray free electron laser (FEL) undulator can be tailored. The characteristic of the amplification of an isolated attosecond pulse in the FEL undulator is investigated. An isolated 180 attoseconds full width half maximum (FWHM) pulse at 1.25 nm with a spectral bandwidth of 1% is injected into an undulator. The simulation results show that for a direct seeding of 3MW, the seed is amplified to the peak power of 106 GW (40 μJ, an output pulse-width of 383 attoseconds) in the presence of a detuning at FEL resonance condition in 100-m long undulator. We note that the introduction of detuning leads to the better performance compared to the case without detuning: shorter by 15.5% in a pulse-width and higher by 76.6% in an output power. Tapering yields a higher power (116% increases in the output power compared to the case without detuning) but a longer pulse (15.4% longer in the pulse-width). It was observed that ± Δλ(r)/8 (Δλ(r)/λ(r) ~1%) is the maximum degree of detuning, beyond which the amplification becomes poor: lower in the output power and longer in the pulse duration. The minimum power for a seed pulse needs to be higher than 1 MW for the successful amplification of an attosecond pulse at 1.25 nm. Also, the electron beam energy-spread must be less than 0.1% for a suitable propagation of attosecond pulse along the FEL undulator under this study.

摘要

我们证明了在X射线自由电子激光(FEL)波荡器中阿秒脉冲的放大可以进行调控。研究了FEL波荡器中孤立阿秒脉冲的放大特性。一个中心波长为1.25nm、半高全宽(FWHM)为180阿秒且光谱带宽为1%的孤立脉冲被注入到一个波荡器中。模拟结果表明,对于3MW的直接种子注入,在100m长的波荡器中,在FEL共振条件下存在失谐时,种子脉冲被放大到峰值功率为106GW(40μJ,输出脉冲宽度为383阿秒)。我们注意到,与无失谐的情况相比,引入失谐会带来更好的性能:脉冲宽度缩短15.5%,输出功率提高76.6%。渐变会产生更高的功率(与无失谐情况相比,输出功率增加116%),但脉冲更长(脉冲宽度长15.4%)。据观察,±Δλ(r)/8(Δλ(r)/λ(r)~1%)是最大失谐程度,超过此程度放大效果变差:输出功率降低,脉冲持续时间变长。对于1.25nm阿秒脉冲的成功放大,种子脉冲的最小功率需要高于1MW。此外,在本研究中,为了使阿秒脉冲沿FEL波荡器顺利传播,电子束能量 spread必须小于0.1%。

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