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Velocity dispersion of correlated energy spread electron beams in the free electron laser

机译:自由电子激光器中相关能量扩散电子束的速度色散

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摘要

The effects of a correlated linear energy/velocity chirp in the electron beam in the free electron laser (FEL), and how to compensate for its effects by using an appropriate taper (or reverse-taper) of the undulator magnetic field, is well known. The theory, as described thus far, ignores velocity dispersion from the chirp in the undulator, taking the limit of a 'small' chirp. In the following, the physics of compensating for chirp in the beam is revisited, including the effects of velocity dispersion, or beam compression or decompression, in the undulator. It is found that the limit of negligible velocity dispersion in the undulator is different from that previously identified as the small chirp limit, and is more significant than previously considered. The velocity dispersion requires a taper which is nonlinear to properly compensate for the effects of the detuning, and also results in a varying peak current (end thus a varying gain length) over the length of the undulator. The results may be especially significant for plasma driven FELs and low energy linac driven FEL test facilities.
机译:众所周知,自由电子激光(FEL)中电子束中线性能量/速度线性调频相关的影响,以及如何通过使用适当的波峰磁场锥度(或反向锥度)来补偿其影响。 。到目前为止,该理论忽略了起伏器中线性调频脉冲的速度色散,取“小”线性调频脉冲的极限。在下文中,重新讨论了补偿光束中线性调频的物理学,包括波荡器中速度分散或光束压缩或解压缩的影响。发现波动器中速度分散的极限可以忽略,与先前确定的小chi极限不同,并且比先前考虑的更为重要。速度色散需要一个锥度,该锥度是非线性的,以适当补偿失谐的影响,并且还导致在波荡器的整个长度上变化的峰值电流(最终是变化的增益长度)。对于等离子体驱动的FEL和低能量直线加速器驱动的FEL测试设备,结果可能尤其重要。

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