环型线电流线极化wiggler

提出一种新型产生线极化摇摆磁场的wiggler,即环型线电流线极化wiggler.它是由许多圆环及连接导线固定在w屯gler骨架上而组成.通过求解拉普拉斯方程,导出了此w电eler磁场分布的理论解.理论解表明,此wiggler产生的线极化磁场不仅在z轴附近空间基模占空比大,而且在垂直于线极化磁场方向能形成具有聚束能力的六极子磁场.此装置的另一特点是容易加工成短周期(5—10mm)wiggler,并且非常容易实现变磁场、变周期和同时变磁场变周期的线极化wiggler.     

一种高性能小周期摇摆器

介绍一种高性能小周期摇摆器的设计。采用槽型定位的分离状磁块,实现了磁场的半周期调节,对该摇摆器模型进行的测量表明,当摇摆器的周期λ_w=10mm,磁极间隙δ为5mm时,峰值磁场B_w=0.35T,磁场最大偏差δB_w/B_w<1.25％。     

光学速调管的研究

用毫米波段的光学速调管结构改进自由电子激光器的增益和效率.编制计算机模拟的程序,用来设计光学速调管装置.对于采用小周期摆动磁场的特定情况,片状电子束电压300keV,电流17A,摆动磁场周期3.7mm,工作频率300GHz,光学速调管的增益和效率分别计算为27.9dB和0.5%.若电子束电压为450keV,电流为25A,磁场周期为1cm,工作频率为160GHz,计算结果增益和效率分别为32dB和2.7%.     

行波管中静态轨迹的研究

 研究了行波管中均匀聚焦磁场和周期永磁聚焦磁场对轨迹波动的影响。推导了这两种磁场下轨迹波动周期和幅值,讨论了磁场强度对轨迹的影响。解释了聚焦磁场存在小的波动的原因,并且通过计算得出小波动的周期为磁场周期的1/2,揭示了在周期永磁聚焦磁场下,电子轨迹近似等效于周期为周期永磁聚焦磁场1/2的小波动和均匀磁场形成的波动轨迹的叠加。利用电子科技大学编写的微波管模拟套装中的3维注-波互作用模块进行了静态轨迹计算,验证了理论推导。     

同轴相对论速调管周期永磁聚焦系统的初步研究

为了探索相对论速调管放大器(RKA)的小型化技术,开展了同轴RKA周期永磁聚焦的物理与设计技术研究。周期永磁聚焦系统采用Halbach阵列结构,产生的磁场类型为周期性会切磁场。首先给出该系统的磁场各个分量的表达式,分析该系统磁场分布的特点,并推导得出该系统聚焦强流环形电子束的稳定条件。根据该稳定条件,对Ka波段同轴RKA设计了一个周期永磁聚焦系统,并优化了周期磁场参数,确定了磁场系统设计的最佳周期和幅值。研究结果显示,周期永磁(PPM)聚焦系统在周期长度18 mm和磁场幅值0.33 T的条件下可引导500 kV、6 kA的同轴RKA,得到1 GW的微波输出功率,物理分析确定了周期永磁聚焦系统应用于高功率同轴RKA的技术可能性。     

一种基于高温超导带材的超导波荡器磁体概念设计

提出了一种新型的可连续绕线的二代高温超导波荡器磁体。波荡器磁体采用"水平跑道型"无绝缘线圈结构,其周期长度为16 mm,绕线带材的宽度为4 mm,厚度为55μm。利用转向器,波荡器磁体的一个绕线槽中的带材可以被引导至相邻的线槽而达到连续绕线的目的。另外,还对此类三周期的波荡器磁体在不同温区,不同带材宽度和不同磁体间隙的条件下的临界电流密度,垂直于带材的磁场和束流中心轴向磁场等参数进行了计算。     

上海光源超导波荡器磁体5周期模型机的研制

上海光源正在研制一台低温超导波荡器模型机,周期数50,周期长度16mm,磁间隙8mm,目标峰值磁场0.88T。首先研制了一台5周期超导波荡器磁体模型机进行技术可行性研究。磁体绕组采用Nb Ti超导线,骨架加工采用电工纯铁。使用传导冷却的测试装置进行了磁体降温、通电与磁场测量。磁体经过两次失超之后达到设计电流值387A。达到的最大电流为433A。当磁体稳定运行在400A时,测得磁场峰值为0.93T。研究结果表明已有的超导磁体关键技术与工艺能够满足50周期超导波荡器模型机的研制需求。     

带状注速调管电子光学系统的设计与模拟

 设计了对有限宽带状注进行聚焦的周期永磁（PPM）磁场，利用E-GUN，SUPERFISH，MAFIA和PIC模拟软件，建立了计算具有平面对称结构的2维及3维电子光学系统模拟平台,并应用此平台对X波段、100 MW带状注速调管的电子光学系统进行了设计与模拟。结果显示，利用设计的PPM聚焦系统，当磁场周期为60 mm，入口处磁场为0.1 T时，在600 mm的传输距离下，电子注的通过率达到了99.6%。     

强磁场混合型短周期摇摆器研究

对混合型短周期摇摆器磁场进行了解析求解,给出了与摇摆器周期、间隙、磁块性能、磁场尺寸以及磁极尺寸等相关的二维解析表达式。根据该公式,作者讨论了混合型短周期摇摆器产生强磁场的潜在能力,提出了一系列改进方法,并分别进行了模型实验,实验结果与理论分析相符合。目前,在1cm周期、5mm间隙的短周期摇摆器模型试验中,中心轴峰值磁感应强度已达到0.45T。另外,该短周期摇摆器可进行单磁场磁场调节,最大峰峰值磁场相对误差小于1％。     

交变极性聚焦磁场抑制Corkscrew运动的机理

 分析了对强流相对论电子束采用交变极性聚焦磁场聚焦存在稳定解的条件,提出了采用交变极性聚焦磁场抑制Corkscrew运动的机理.数值计算结果表明,在采用交变周期为1m、峰值磁场设为0.2T的情况下,对于能量为12MeV的电子束,当聚焦布局长度为2.8m时,束质心位移可从5mm（始端）被抑制至近似0 (终端);对于能量为20MeV的电子束,当聚焦布局长度为4.5m时,束质心位移可从5mm（始端）被抑制至近似0(终端)。     

Mode-selective amplification in a waveguide free electron laserwith a two-sectioned wiggler

One important issue in waveguide free electron lasers (FELs) involves an interaction of the electron beam with one waveguide mode at two different resonant frequencies. Since the low-frequency mode often has a higher pain, the usually preferred high-frequency mode is suppressed as a result of mode competition. In this paper, possible control of this mode competition is considered using a nonstandard wiggler magnet consisting of two cascaded wiggler sections with different periods and field strengths. It is demonstrated that with an appropriate differentiation between the two wiggler sections the high-frequency mode may be amplified preferentially. This mode-selective amplification may be used to suppress the low-frequency mode. A small signal gain formulation is developed for a waveguide FEL with such a two-sectioned wiggler arrangement and numerical examples are used to demonstrate its applicability to mode control in waveguide FELs. Effects of wiggler field errors and electron energy spread are also considered. It is shown that the requirement for wiggler field errors and electron energy spread in the two-sectioned wiggler arrangement is similar to that in the usual straight wiggler configuration     

RELATIONSHIP BETWEEN THE SPONTANEOUS AND THE STIMULATED RADIATIONS IN A NOVEL WIGGLER FREE-ELECTRON LASER

The spontaneous and the stimulated radiations, as well as the relationship between them, are calculated for an electron moving in the wiggler with the independent magnetostatic-field on the axial (z) coordinates. It is shown that the Madey's law is still valid in the novel wiggler case. The small signal gain of free-clectron laser is calculated in a novel wiggler.     

Plasma Induced Wiggler Magnetic Field in a Cavity

The transformation of an elliptically polarized standing wave in a cavity by a suddenly and uniformly created plasma is discussed. Theoretical expressions for the plasma induced wiggler magnetic field as well as the frequency-upshifted standing wave are derived. By choosing appropriate values of the source wave parameters and plasma parameters, one can get wiggler magnetic field of desired magnitude, direction and wiggler wavelength. A few representative results are discussed.     

第一台真空内扭摆磁铁的设计与研制

主要介绍了北京正负电子对撞机上为提高同步辐射光源性能而设计建造的第一台真空内扭摆磁铁的概况,论述了真空内扭摆磁铁的设计要求和参数,以及研制过程中的关键技术和难度,并且给出了相应的磁场测量结果     

The Magnetic Field Distributions and Beam Propagation Properties of the Hybrid Coaxial Wiggler

In this paper a novel coaxial wiggler, the hybrid coaxial wiggler, is proposed. The analytical formula for magnetic field of the wiggler is derived, and the beam propagation properties are investigated numerically. The results show that the hybrid coaxial wiggler is scalable to small periods with high field amplitude, high beam current acceptance, and excellent transverse focusing properties.     

A multipole superconducting wiggler for Canadian light source

A contract for multipole superconducting wiggler design and fabrication between The University of Saskatchewan and Budker Institute of Nuclear Physics was signed in October 2003. A wiggler with the photons energy range 4 to 40 keV, the maximum field 1.9 T, and the period length as small as possible was required for the micro-XAFS beamline. In 2004 the 2 T 63-pole superconducting wiggler with the average period length 34 mm was fabricated in BINP. To eliminate the undulator-type spectrum, the periodicity of the wiggler was broken. A new approach to the cryostat design enabled long-time (up to 6 months) machine operation without liquid helium refilling (LHe consumption <0.03 l/h). After successful tests the wiggler was installed on the Canadian Light Source (CLS) storage ring with the energy 2.9 GeV in January 2005. The main parameters of the magnet and the cryogenic systems, as well as magnet measurements data, cryogenic system test data, and experimental results during machine operation on the CLS storage ring are presented.     

Experimental and numerical studies of sheet electron beampropagation through a planar wiggler magnet

Detailed experimental studies on sheet relativistic electron beam propagation through a long planar wiggler are reported and compared with numerical simulations. The planar wiggler has 56 periods with a period of 9.6 mm. Typically, the wiggler field peak amplitude is 5 kG. The experimental efforts are focused on controlling the deviation of the beam toward the side edge of the planar wiggler along the wide transverse direction. It is found that a suitably tapered magnetic field configuration at the wiggler entrance can considerably reduce the rate of deviation. The effects of the following techniques on beam transport efficiency are discussed: side focusing, beam transverse velocity tuning at the wiggler entrance, and beam spread limiting. High beam transport efficiency (almost 100%) of a 15-A beam is obtained in some cases     

Electron acceleration in the inverse free electron laser with a helical wiggler by axial magnetic field and ion-channel guiding

Electron acceleration in the inverse free electron laser (IFEL) with a helical wiggler in the presence of ion-channel guiding and axial magnetic field is investigated in this article. The effects of tapering wiggler amplitude and axial magnetic field are calculated for the electron acceleration. In free electron lasers, electron beams lose energy through radiation while in IFEL electron beams gain energy from the laser. The equation of electron motion and the equation of energy exchange between a single electron and electromagnetic waves are derived and then solved numerically using the fourth order Runge-Kutta method. The tapering effects of a wiggler magnetic field on electron acceleration are investigated and the results show that the electron acceleration increases in the case of a tapered wiggler magnetic field with a proper taper constant.     

毫米波自由电子激光的数值模拟和实验的比较

从波导管毫米波自由电子激光器的设计要求出发,根据Livermore实验室FRED程序的物理思想,编制了空间三维的数值模拟程序(WAGFEL)。为了检验程序的可靠程度,结合ELF装置的实际参数,进行了数值模拟并和实验结果进行了比较。结果表明,把Wiggler磁场B_w增大300 Gs后,WAGFEL程序的模拟结果和Livermore实验室的实验结果基本符合。模拟使用的全部参数,除B_w增大300Gs外,都是ELF的实际参数。模拟时峰值磁场B_w=4050Gs,实验测量峰值磁场B_w=3720Gs,相差在8％左右。WAGFEL程序可以用来从事毫米波自由电子激光器的设计以及基本物理问题的研究。     

圆柱螺旋电磁Wiggler的场形分析

 利用载流圆柱螺旋线系统内部的磁标势满足的Laplace方程, 以及系统磁矢势的积分形式, 定出Laplace方程通解的未知系数, 求得左(右)旋单绕圆柱螺旋线的磁标势。应用磁场的叠加原理以及积分法, 给出了各种类型如双绕、双双绕、交叉绕等螺旋形Wiggler的场形分布公式。