论文标题

自由电子激光器的变化极化控制

Variable Polarization Control in Free-Electron Lasers

论文作者

Freund, H. P., van der Slot, P. J. M.

论文摘要

自由电子激光器(FELS)几乎在整个电磁光谱上从微波炉穿过紫外线到紫外线,而硬X射线是播种或从噪声开始的。 FELS可以根据所使用的波动器的特性产生各种输出辐射的各种不同的光学极化。例如,X射线FEL使用由一系列相对较短的波动器组成的长起伏线。由于制造和调整的易用性,大多数这样的fel使用线性极化的波动器。因此,光输出是线性极化的。但是,通过改变线路沿线的方向,可以通过改变椭圆形或圆形极化。或者,Apple-II或Delta Ouldurotator设计允许产生具有任意极化的起伏的磁场。在这里,我们提出了一个三维,时间依赖性的公式,该公式会自以为是模拟了两个独立的光学极化,因此,完全处理了未驱动器,解散器缺陷和下降器降解的任何给定的序列或组合,配方的两个原理特性具有两个构成这种能力的原理特征。首先,使用波动器场的三维分析模型,通过完整的洛伦兹力方程进行了粒子轨迹。这允许电子与各种不同的漏斗场和方向的相互作用的准确模型。第二,该公式使电子可以同时将电磁波的两个独立极化搭配在一起,因此允许光学偏振沿波动器线自兼而有。在首次描述数值模型之后,我们开始使用感兴趣的不同悬端配置给出一些示例。

Free-electron lasers (FELs) over virtually the entire electromagnetic spectrum from microwaves through ultraviolet through hard x-rays that are either seeded or start from noise. FELs can produce a variety of different optical polarizations of the output radiation ranging from linear through elliptic to circular polarization depending upon the characteristics of the undulators used. For example, x-ray FELs use long undulator lines composed of a series of relatively short undulators. Most such FELs use linearly polarized undulators due to the ease of manufacture and tuning; hence the optical output is linearly polarized. However, elliptic or circular polarizations are possible by varying the orientation of the undulators along the line. Alternately, APPLE-II or Delta undulator designs allow for producing undulating magnetic fields with arbitrary polarizations. Here, we present a three-dimensional, time-dependent formulation that self-consistently models two independent optical polarizations and, therefore, completely treats any given sequence or combination of undulator, undulator imperfections, and undulator degradation There are two principal characteristics of the formulation that underpin this capability. In the first place, the particle trajectories are integrated by means of the full Lorentz force equations using three-dimensional analytic models of the undulators fields. This permits an accurate model of the interaction of the electrons with a large variety of undulator fields and orientations. In the second place, the formulation allows the electrons to couple simultaneously to two independent polarizations of the electromagnetic wave and, therefore, allows the optical polarization to evolve self-consistently along the undulator line. After first describing the numerical model, we proceed to give some examples using different undulator configurations that are of interest.

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