波导范霍夫奇点附近电子回旋运动的经典辐射阻尼增强

IF 4.3 3区 材料科学 Q1 ENGINEERING, ELECTRICAL & ELECTRONIC
Yuki Goto, Savannah Garmon, Tomio Petrosky
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引用次数: 0

摘要

我们利用经典的弗里德里希斯模型研究了电子回旋运动的阻尼过程以及由此在波导中产生的发射,而不依赖于费米黄金定律等扰动分析。范霍夫奇点出现在与波导中每种电磁场模式相关的色散下限(或截止频率)处。我们发现,在范霍夫奇点附近,不仅与共振极相关的衰减过程会增强(放大系数 ∼104),而且支点效应也会相应增强。因此,大部分衰变发生的时间尺度大大缩短。此外,这表明在范霍夫奇点附近应该可以通过实验观测到非马尔可夫分支点效应。我们的处理方法产生了一个物理上可接受的解,而不会出现众所周知的基于亚伯拉罕-洛伦兹方程的经典辐射阻尼传统处理方法中出现的失控解问题。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Enhanced classical radiation damping of electronic cyclotron motion in the vicinity of the Van Hove singularity in a waveguide
We study the damping process of electron cyclotron motion and the resulting emission in a waveguide using the classical Friedrichs model without relying on perturbation analysis such as Fermi’s golden rule. A Van Hove singularity appears at the lower bound (or cut-off frequency) of the dispersion associated with each of the electromagnetic field modes in the waveguide. In the vicinity of the Van Hove singularity, we found that not only is the decay process associated with the resonance pole enhanced (amplification factor ∼104) but the branch-point effect is also comparably enhanced. As a result, the timescale on which most of the decay occurs is dramatically shortened. Further, this suggests that the non-Markovian branch point effect should be experimentally observable in the vicinity of the Van Hove singularity. Our treatment yields a physically-acceptable solution without the problematic runaway solution that is well known to appear in the traditional treatment of classical radiation damping based on the Abraham-Lorentz equation.
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来源期刊
CiteScore
7.20
自引率
4.30%
发文量
567
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