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中国科学技术大学 国家同步辐射实验室 合肥 230022
[ "李成龙,男,1987年出生,2010年毕业于中国科技大学,现为硕士研究生,核科学与技术专业", "LI Chenglong, male, born in 1987, graduated from University of Science and Technology of China in 2010, master student, major in nuclear science and technique" ]
收稿日期:2016-04-05,
修回日期:2016-05-17,
纸质出版日期:2016-09
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李成龙, 汤振兴, 裴元吉. 低发射度L波段光阴极微波电子枪物理设计[J]. 核技术, 2016,39(9):090203
Chenglong LI, Zhenxing TANG, Yuanji PEI. Physical design of low-emittance L-band photocathode microwave electron gun[J]. Nuclear techniques, 2016, 39(9): 090203
李成龙, 汤振兴, 裴元吉. 低发射度L波段光阴极微波电子枪物理设计[J]. 核技术, 2016,39(9):090203 DOI: 10.11889/j.0253-3219.2016.hjs.39.090203.
Chenglong LI, Zhenxing TANG, Yuanji PEI. Physical design of low-emittance L-band photocathode microwave electron gun[J]. Nuclear techniques, 2016, 39(9): 090203 DOI: 10.11889/j.0253-3219.2016.hjs.39.090203.
太赫兹(THz)光源对电子束的能量、能散及发射度有极高要求,研发高性能电子源是基于自由电子激光(Free Electron Laser
FEL)的THz光源的重要挑战。对电子腔中束团发射度增长机制的研究,有助于设计针对有效的发射度补偿方案。本文首先描述了L波段光阴极微波电子枪腔的设计,利用POISSON Superfish软件给出了腔内电磁场分布,详细分析了束流发射度增长的因素,讨论发射度补偿原理。由此提出基于主副螺线管线圈抑制发射度增长的补偿方案,并用ASTRA程序对补偿效果进行模拟计算。结果表明,采用该补偿方案后,电子腔输出束团的能散和发射度有显著改善,达到THz光源对于电子源的要求。
Background:
2
The development of high performance electron beam source has been a challenge for Free-electron Laser(FEL)based THz source which is critical for the energy
energy spread and emittance of the electron beam.
Purpose:
2
This work aims to find out the mechanism of emittance growth and developing a compensation technique for this emittance growth in the Radio Frequency(RF)gun cavity.
Methods:
2
First of all
a RF gun cavity is designed using POISSON Superfish to calculate its electro-magnetic field distribution for analysis of the emittance growth mechanism.Then
a compensation scheme is developed by employing a pair of solenoids to reduce the space charge emittance.Finally
the effectiveness of scheme is evaluated using the commonly used reliable simulation program ASTRA.
Results:
2
The simulation results show that the normalized transverse emittance of a 5.67-MeV electron bunch with 200 pC is reduced to 0.373 mm·mrad while the energy spread is reduced to 2.3‰.For a 5.67-MeV electron bunch with 1000 pC
the emittance and energy spread are reduced to 0.934 mm·mrad and 7.6‰
respectively.
Conclusion:
2
Simulation of the final design shows that the performance of the electron beam produced by the RF gun has achieved the requirements for THz source.
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