共查询到17条相似文献,搜索用时 250 毫秒
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提出一种新的紧凑型强流电子枪结构。紧凑型自聚束微波电子枪是一个多驻波腔结构,最大特点是腔与腔之间相互没有耦合,每腔可分别独立馈入功率和调节相位。通过选择合适的馈入功率和高频相位搭配,能够得到较优的束流品质。在此基础上采用外注入电子束的结构,能进一步增大流强和降低能散度,同时消除电子反轰对阴极工作的不利影响。利用Superfish和Parmela程序对腔体结构和束流动力学反复进行计算,确定了一组结构和工作参数。模拟结果表明出束微脉冲峰值流强可以到18 A,能散度小于2‰,横向发射度小于6 πmm·mrad。最后给出腔体冷侧结果,与模拟计算结果吻合得较好。 相似文献
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采用URMEL-T程序进行了二次发射微波电子枪的腔内电磁计算和特性分析。同时利用URMEL-T得出的腔内轴向电场及自编程序,模拟电子在该高频场作用下的运动。计算表明二次发射微波电子枪确实具有相位选择性,进而探讨了腔形尺寸、射频电场强度对相位选择性和产生二次倍增的有关条件的影响,以及输出电子的能量稳定性。模拟结果表明,这类电子枪(MPG)可得到高电流密度(5303A/cm2)及短脉冲(3.15~10ps)的电子束。 相似文献
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模拟研究了1.6个腔、高梯度的W-band光阴极微波电子枪系统,该系统能产生和加速300pC的电子束团.设计系统由频率91.392GHz光阴极微波电子枪以及频率91.392GHz行波加速结构组成.基于射频直线加速器标度律与数值模拟结果,设计系统能产生能量1.74MeV,电量300pC,束团长度0.72ps,归一化横向发射度0.55mm·mrad的电子束团.研究了高频、高梯度下的束流动力学.由于高梯度,有质动力效应在束流动力学中起重要作用,且由于横向与纵向之间的耦合,在基次空间谐波的情形下,仍然存在着有质动力聚焦效应. 相似文献
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注入器设计过程中主要关注的指标有微脉冲束流强度、电子能量、电子束能散度、反轰功率和发射度等。为了满足自由电子激光研究的需要,要求峰值流强大于5A。由于热阴极微波电子枪存在电子反轰,束流负载效应将引起能散度的增加,因此为了降低能散度,要求尽量降低反轰。利用Suoerfish程序进行了腔形优化设计,分析了加速腔内的电场分布,计算了腔壁的损耗。利用Parmela程序进行了束流动力学计算。为了提高首腔的电子俘获系数,减小电子反轰,设计过场中采用了缩短首腔长度, 相似文献
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根据新型分析扫描电子显微镜的工作原理及载能电子束和固体相互作用原理,利用蒙特卡罗方法模拟入射电子和靶物质的相互作用过程,编制了蒙特卡罗模拟计算程序,获得了对应不同电镜工作参数的入射电子背散射率. 相似文献
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The ADS (accelerator driven subcritical system) project was proposed by the Chinese Academy of Sciences. The initial proton beams delivered from an electron cyclotron resonance ion source can be effectively accelerated by 162.5 MHz 4.2 m long room temperature radio-frequency-quadrupoles (RFQ) operating in CW mode. To test the feasibility of this physical design, a new Fortran code for RFQ beam dynamics study, which is space charge dominated, was developed. This program is based on Particle-In-Cell (PIC) technique in the time domain. Using the RFQ structure designed for the CADS project, the beam dynamics behavior is performed. The well-known simulation code TRACK is used for benchmarks. The results given by these two codes show good agreements. Numerical techniques as well as the results of beam dynamics studies are presented in this paper. 相似文献
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Yong-Chun Feng Rui-Shi Mao Peng Li Xin-Cai Kang Yan Yin Tong Liu Yao-Yao You Yu-Cong Chen Tie-Cheng Zhao Zhi-Guo Xu Yan-Yu Wang You-Jin Yuan 《中国物理C(英文版)》2017,41(7):077001-077001
An electron beam probe(EBP) is a detector which makes use of a low-intensity and low-energy electron beam to measure the transverse profile, bunch shape, beam neutralization and beam wake field of an intense beam with small dimensions. While it can be applied to many aspects, we limit our analysis to beam distribution reconstruction.This kind of detector is almost non-interceptive for all of the beam and does not disturb the machine environment.In this paper, we present the theoretical aspects behind this technique for beam distribution measurement and some simulation results of the detector involved. First, a method to obtain a parallel electron beam is introduced and a simulation code is developed. An EBP as a profile monitor for dense beams is then simulated using the fast scan method for various target beam profiles, including KV distribution, waterbag distribution, parabolic distribution,Gaussian distribution and halo distribution. Profile reconstruction from the deflected electron beam trajectory is implemented and compared with the actual profile, and the expected agreement is achieved. Furthermore, as well as fast scan, a slow scan, i.e. step-by-step scan, is considered, which lowers the requirement for hardware, i.e. Radio Frequency deflector. We calculate the three-dimensional electric field of a Gaussian distribution and simulate the electron motion in this field. In addition, a fast scan along the target beam direction and slow scan across the beam are also presented, and can provide a measurement of longitudinal distribution as well as transverse profile simultaneously. As an example, simulation results for the China Accelerator Driven Sub-critical System(CADS) and High Intensity Heavy Ion Accelerator Facility(HIAF) are given. Finally, a potential system design for an EBP is described. 相似文献
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对一个新型、紧凑、高效的电子直线加速器的加速管的设计,进行了等阻抗与等梯度两种结构的比较研究.对于使用一个5MW速调管的能量和相位经过选择的用毕束流注入到两种加速管的情况应用Parmela程序进行了模拟计算.说明宜于加工和调试的等阻抗加速管更为适宜.最后,简单地讨论了如用更高功率(如30MW?,相应加速能量约为30MeV)的速调管用毕束流作为这种新型加速器的注入束时,等阻抗加速结构除了在设计、加工、调试中的简单易行外,同时模拟结果表明整个加速管无需外加横向聚焦磁场. 相似文献