W波段同轴静磁波荡器自由电子激光优化设计

基于同轴静磁波荡器的自由电子激光主要利用环形电子束与同轴TE模式的相互作用产生电磁辐射,是一种重要的毫米波辐射源。分析了同轴结构作用区内外半径、工作模式、电子束电压、波荡器周期等参数对辐射频率的影响规律,研究了电子束平均半径的选取原则和束波互作用腔的设计方法,设计了辐射频率在W波段的基于同轴静磁波荡器的自由电子激光,并进行了粒子模拟,在电子束电压为720 kV,电子束流为1 kA的情况下,获得了频率107 GHz、辐射功率35 MW的TE01模,束波转换效率为4.9%,束波作用腔总长度小于200 mm,同轴静磁波荡器的磁场幅度0.34 T。     

兼用FEL光学速调管的同步辐射波荡器的设计

介绍了合肥８００ＭｅＶ储存环ＦＥＬ光学速调管改造成同步辐射波荡器的设计与计算过程，给出了改造方法，计算了波荡器的光通量与亮度并给出了光通量与亮度曲线．计算结果表明，改造后的波荡器可以将目前辐射亮度提高两个多数量级，使许多目前光源亮度下无法开展的研究工作得以进行．     

可变椭圆极化波荡器相干太赫兹辐射的模拟计算

中国科学院上海应用物理研究所正在研制的相干太赫兹辐射装置是一台利用飞秒电子束团通过可变椭圆极化波荡器产生高亮度水平线极化光、垂直线极化光或各种椭圆极化光的强相干太赫兹辐射光源.本文描述了这种相干太赫兹辐射的光通量密度空间分布、光谱、极化特性和相干性等的计算方法和模拟计算结果.计算结果表明,对于能量为20MeV、发射度为15πmm·mrad、束团长度为200fs、电荷量为50pC的电子束团,在距离0.6m长的波荡器中心1m处可获得光通量密度峰值达2×10⁹photons/mm²/0.1%bw量级的太赫兹水平线极化光或圆极化光     

Crystalline undulator radiation and sub-harmonic bifurcation of system

Looking for new light sources, especially short wavelength laser light sources has attracted widespread attention. This paper analytically describes the radiation of a crystalline undulator field by the sine-squared potential. In the classical mechanics and the dipole approximation, the motion equation of a particle is reduced to a generalized pendulum equation with a damping term and a forcing term. The bifurcation behavior of periodic orbits is analyzed by using the Melnikov method and the numerical method, and the stability of the system is discussed. The results show that, in principle, the stability of the system relates to its parameters, and only by adjusting these parameters appropriately can the occurrence of bifurcation be avoided or suppressed.     

波荡器对电子储存环束流影响的研究

研究了国家同步辐射实验室二期工程新建波荡器对储存环束流产生的各种影响,计论了在高亮度模式下,波荡器产生的效应。结果表明：波荡器安装在第三直线节在两种工作模式下对环的影响都有小,不影响正常运行,无须补偿。但安装在第四直线节时,在高亮度运行模式下对电子束流的影响较大,如不进行补偿,环将无法正常运行。     

Observation of an optical vortex beam from a helical undulator in the XUV region

The observation of an optical vortex beam at 60 nm wavelength, produced as the second‐harmonic radiation from a helical undulator, is reported. The helical wavefront of the optical vortex beam was verified by measuring the interference pattern between the vortex beam from a helical undulator and a normal beam from another undulator. Although the interference patterns were slightly blurred owing to the relatively large electron beam emittance, it was possible to observe the interference features thanks to the helical wavefront of the vortex beam. The experimental results were well reproduced by simulation.     

晶体摆动场的辐射衰减与能量增益

由于晶体弯曲、电子多重散射和晶格热振动引起的粒子退道,辐射同原子相互作用引起的电离损失,以及系统非线性引起的全局分叉与混沌行为等,晶体摆动场辐射面临的问题比自由电子激光要复杂得多。首先,引入晶体摆动场自发辐射谱分布,并在简谐近似下讨论了运动方程、系统增益和能量衰减。结果表明:一般情况下辐射谱只有少数几条谱线,而在简谐近似下,谱线只有一条。其次,指出了辐射能量比较高时,衰减是主要的,选择的晶体长度必须小于衰减长度,且可选择正电子或质子作炮弹;当辐射能量比较低时,退道是主要的,选择的晶体长度必须小于退道长度,且可选择重离子作炮弹。     

Optimization of the lattice function in the planar undulator applied for terahertz FEL oscillators

Since the beta function of the electron beam within the undulator has a great influence on the power gain of the free electron laser (FEL), optimization of the undulator lattice becomes important. In this paper, the transfer matrix of the planar undulator is obtained from differential equations of the electron motion. Based on this, the lattice function of the planar undulator in a terahertz FEL oscillator proposed by Huazhong University of Science and Technology (HUST-FEL) is optimized and the expressions of the average beta function are derived. The accuracy of the optimization result was confirmed well by the numerical method. The application range of this analytical method is given as well. At last, the emittance growth in the horizontal direction due to the attenuation of the magnetic field is discussed.     

Characteristics of a tapered undulator for the X‐ray absorption fine‐structure technique at PLS‐II

An in‐vacuum undulator (IVU) with a tapered configuration was installed in the 8C nanoprobe/XAFS beamlime (BL8C) of the Pohang Light Source in Korea for hard X‐ray nanoprobe and X‐ray absorption fine‐structure (XAFS) experiments. It has been operated in planar mode for the nanoprobe experiments, while gap‐scan and tapered modes have been used alternatively for XAFS experiments. To examine the features of the BL8C IVU for XAFS experiments, spectral distributions were obtained theoretically and experimentally as functions of the gap and gap taper. Beam profiles at a cross section of the X‐ray beam were acquired using a slit to visualize the intensity distributions which depend on the gap, degree of tapering and harmonic energies. To demonstrate the effect of tapering around the lower limit of the third‐harmonic energy, V K‐edge XAFS spectra were obtained in each mode. Owing to the large X‐ray intensity variation around this energy, XAFS spectra of the planar and gap‐scan modes show considerable spectral distortions in comparison with the tapered mode. This indicates that the tapered mode, owing to the smooth X‐ray intensity profile at the expense of the highest and most stable intensity, can be an alternative for XAFS experiments where the gap‐scan mode gives a considerable intensity variation; it is also suitable for quick‐XAFS scanning.     

The E166 experiment: Development of an undulator-based polarized positron source for the international linear collider

A longitudinal polarized positron beam is foreseen for the international linear collider (ILC). A proof-of-principle experiment has been performed in the final focus test beam at SLAC to demonstrate the production of polarized positrons for implementation at the ILC. The E166 experiment uses a 1 m long helical undulator in a 46.6 GeV electron beam to produce a few MeV photons with a high degree of circular polarization. These photons are then converted in a thin target to generate longitudinally polarized e ⁺ and e ⁻. The positron polarization is measured using a Compton transmission polarimeter. The data analysis has shown asymmetries in the expected vicinity of 3.4% and ∼1% for photons and positrons respectively and the expected positron longitudinal polarization is covering a range from 50% to 90%.