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Slice emittance and projected emittance
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作者 李正红 《Chinese Physics B》 SCIE EI CAS CSCD 2008年第3期901-907,共7页
This paper presents an analytical description for the growth of the projected emittanee (here just referred to the transverse emittance) based on the concept of the slice emittance in an RF photoinjector. In the RF ... This paper presents an analytical description for the growth of the projected emittanee (here just referred to the transverse emittance) based on the concept of the slice emittance in an RF photoinjector. In the RF photoinjector, the slice emittance undergoes small changes, but the projected emittance changes significantly even in the drift space after the injector. Carefully adjusting the parameters of the RF photoinjector, which usually means emittance compensation, the projected emittance can be minimized to the value of the slice emittance. The relation between slice emittance and projected emittance is explained in this paper. An emittance function, which shows such a relation, is also introduced. A model about the emittance growth in the RF photoinjector is established, which accords with the particle simulation results by using the code ASTRA. The condition to minimize the emittance is also given by using the emittance function, which means the emittance compensation in the RF photoinjector. 展开更多
关键词 PHOTOINJECTOR emittance slice emittance emittance compensation
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High-brightness photo-injector with standing-wave buncher-based ballistic bunching scheme for inverse Compton scattering light source
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作者 Jian-Xin Wang Kui Zhou +7 位作者 Peng Li De-Xin Xiao Li-Jun Shan Xu-Ming Shen Yu Liu Zheng Zhou Han-Bin Wang Dai Wu 《Nuclear Science and Techniques》 SCIE EI CAS CSCD 2022年第4期51-61,共11页
We report our recent progress in the design and simulation of a high-brightness S-band photo-injector with a ballistic bunching scheme aimed at driving an inverse Compton scattering(ICS)X-ray source.By adding a short ... We report our recent progress in the design and simulation of a high-brightness S-band photo-injector with a ballistic bunching scheme aimed at driving an inverse Compton scattering(ICS)X-ray source.By adding a short standing-wave buncher between the RF gun and first booster in a conventional S-band photo-injector,electron bunches with a 500 pC charge can be compressed to the sub-picosecond level with very limited input RF power and an unchanged basic layout of the photo-injector.Beam dynamics analysis indicates that fine tuning of the focusing strength of the gun and linac solenoid can well balance additional focusing provided by the standing wave buncher and generate a well-compensated transverse emittance.Thorough bunching dynamics simulations with different operating conditions of the buncher show that a buncher with more cells and a moderate gradient is suitable for simultaneously obtaining a short bunch duration and low emittance.In a typical case of a 9-cell buncher with a 38 MV/m gradient,an ultrashort bunch duration of 0.5 ps(corresponding to a compression ratio of>5)and a low emittance of<1 mm mrad can be readily obtained for a 500 pC electron pulse.This feasible ballistic bunching scheme will facilitate the implementation of an ultrashort pulse mode inverse Compton scattering X-ray source on most existing S-band photo-injectors. 展开更多
关键词 Beam brightness Ballistic bunching emittance compensation Compton scattering X-ray source
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Velocity bunching in travelling wave accelerator with low acceleration gradient 被引量:1
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作者 黄瑞萱 何志刚 +1 位作者 李伟伟 贾启卡 《Chinese Physics C》 SCIE CAS CSCD 2014年第5期98-102,共5页
We present the analytical and simulated results of our study of the influence of the acceleration gradient in the velocity bunching process, which is a bunch compression scheme that uses a travelling wave accelerating... We present the analytical and simulated results of our study of the influence of the acceleration gradient in the velocity bunching process, which is a bunch compression scheme that uses a travelling wave accelerating structure as a compressor. Our study shows that the bunch compression application with low acceleration gradient is more tolerant to phase jitter and more successful in obtaining a compressed electron beam with symmetrical longitudinal distribution and low energy spread. We also present a transverse emittance compensation scheme to compensate the emittance growth caused by the increase of the space charge force in the compressing process, which is easy to adjust for different compression factors. 展开更多
关键词 travelling wave accelerating structure velocity bunching acceleration gradient emittance compensation
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