Comment on “Quantum effects in spontaneous emission by a relativistic, undulating electron beam” by Robb G. R. M. and Bonifacio R.

G. Geloni, V. Kocharyan, E. Saldin
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引用次数: 5

Abstract

In a recent letter, Robb and Bonifacio [1] claimed that a previously neglected quantum effect results in noticeable changes in the evolution of the energy distribution associated with spontaneous emission in long undulators. They revisited theoretical models used to describe the emission of radiation by relativistic electrons as a continuous diffusive process, and claimed that a drift-diffusion approach can only be used when the parameter =Nw ω/(γmc ) is much smaller than unity, whereNw is the number of undulator periods, is the reduced Planck constant, ω is the photon frequency, γ the relativistic Lorentz factor, m the electron rest mass and c the speed of light. In that work it is argued that when 1, a drift-diffusion equation is no more sufficient to describe the evolution of the distribution of electron momenta, which “occurs as discrete momentum groups according to a Poisson distribution”. However, these results are based on a one-dimensional model of the spontaneous radiation emission. Such model does not account for the angular distribution of the radiation, but only for the emission on axis, which is characterized by an overall relative bandwidth ∼ 1/Nw. In contrast to this, the electron recoil related with the quantized nature of photons depends on the entire angular
对Robb G. R. M.和Bonifacio R.的“相对论性波动电子束自发辐射中的量子效应”的评论。
在最近的一封信中,Robb和Bonifacio[1]声称,以前被忽视的量子效应导致长波动体中与自发发射相关的能量分布的演变发生了显著变化。他们重新研究了用于描述相对论电子辐射发射为连续扩散过程的理论模型,并声称漂移扩散方法只能在参数=Nw ω/(γmc)远小于1时使用,其中enw是波动周期数,是约简普朗克常数,ω是光子频率,γ是相对论洛伦兹因子,m是电子静止质量,c是光速。在该工作中,有人认为当1时,漂移-扩散方程不再足以描述电子动量分布的演变,电子动量“根据泊松分布作为离散动量群出现”。然而,这些结果是基于自发辐射发射的一维模型。这种模型不考虑辐射的角分布,而只考虑轴上的发射,其特征是总体相对带宽为1/Nw。与此相反,与光子量子化性质有关的电子反冲取决于整个角度
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