Back-streaming ion emission and beam focusing on high power linear induction accelerator

Ions released from target surfaces by impact of a high intensity and current electron beam can be accelerated and trapped in the beam potential, and further destroy the beam focus. By solving the 2D Poisson equation, we found that the charge neutralization factor of the ions to the beam under space...

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Main Authors: Jun Zhu, Nan Chen, Haijun Yu, Xiaoguo Jiang, Yuan Wang, Wenhua Dai, Feng Gao, Minhong Wang, Jin Li, Jinshui Shi
Format: Article
Language:English
Published: American Physical Society 2011-08-01
Series:Physical Review Special Topics. Accelerators and Beams
Online Access:http://doi.org/10.1103/PhysRevSTAB.14.082801
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spelling doaj-803372d5e2044d82b3c7dfb8e7cf8ce22020-11-25T01:58:59ZengAmerican Physical SocietyPhysical Review Special Topics. Accelerators and Beams1098-44022011-08-0114808280110.1103/PhysRevSTAB.14.082801Back-streaming ion emission and beam focusing on high power linear induction acceleratorJun ZhuNan ChenHaijun YuXiaoguo JiangYuan WangWenhua DaiFeng GaoMinhong WangJin LiJinshui ShiIons released from target surfaces by impact of a high intensity and current electron beam can be accelerated and trapped in the beam potential, and further destroy the beam focus. By solving the 2D Poisson equation, we found that the charge neutralization factor of the ions to the beam under space charge limited condition is 1/3, which is large enough to disrupt the spot size. Therefore, the ion emission at the target in a single-pulse beam/target system must be source limited. Experimental results on the time-resolved beam profile measurement have also proven that. A new focus scheme is proposed in this paper to focus the beam to a small spot size with the existence of back-streaming ions. We found that the focal spot will move upstream as the charge neutralization factor increases. By comparing the theoretical and experimental focal length of the Dragon-I accelerator (20 MeV, 2.5 kA, 60 ns flattop), we found that the average neutralization factor is about 5% in the beam/target system.http://doi.org/10.1103/PhysRevSTAB.14.082801
collection DOAJ
language English
format Article
sources DOAJ
author Jun Zhu
Nan Chen
Haijun Yu
Xiaoguo Jiang
Yuan Wang
Wenhua Dai
Feng Gao
Minhong Wang
Jin Li
Jinshui Shi
spellingShingle Jun Zhu
Nan Chen
Haijun Yu
Xiaoguo Jiang
Yuan Wang
Wenhua Dai
Feng Gao
Minhong Wang
Jin Li
Jinshui Shi
Back-streaming ion emission and beam focusing on high power linear induction accelerator
Physical Review Special Topics. Accelerators and Beams
author_facet Jun Zhu
Nan Chen
Haijun Yu
Xiaoguo Jiang
Yuan Wang
Wenhua Dai
Feng Gao
Minhong Wang
Jin Li
Jinshui Shi
author_sort Jun Zhu
title Back-streaming ion emission and beam focusing on high power linear induction accelerator
title_short Back-streaming ion emission and beam focusing on high power linear induction accelerator
title_full Back-streaming ion emission and beam focusing on high power linear induction accelerator
title_fullStr Back-streaming ion emission and beam focusing on high power linear induction accelerator
title_full_unstemmed Back-streaming ion emission and beam focusing on high power linear induction accelerator
title_sort back-streaming ion emission and beam focusing on high power linear induction accelerator
publisher American Physical Society
series Physical Review Special Topics. Accelerators and Beams
issn 1098-4402
publishDate 2011-08-01
description Ions released from target surfaces by impact of a high intensity and current electron beam can be accelerated and trapped in the beam potential, and further destroy the beam focus. By solving the 2D Poisson equation, we found that the charge neutralization factor of the ions to the beam under space charge limited condition is 1/3, which is large enough to disrupt the spot size. Therefore, the ion emission at the target in a single-pulse beam/target system must be source limited. Experimental results on the time-resolved beam profile measurement have also proven that. A new focus scheme is proposed in this paper to focus the beam to a small spot size with the existence of back-streaming ions. We found that the focal spot will move upstream as the charge neutralization factor increases. By comparing the theoretical and experimental focal length of the Dragon-I accelerator (20 MeV, 2.5 kA, 60 ns flattop), we found that the average neutralization factor is about 5% in the beam/target system.
url http://doi.org/10.1103/PhysRevSTAB.14.082801
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