Electron trapping and acceleration by the plasma wakefield of a self-modulating proton beam

被引:28
|
作者
Lotov, K. V. [1 ,2 ]
Sosedkin, A. P. [1 ,2 ]
Petrenko, A. V. [1 ,3 ]
Amorim, L. D. [4 ]
Vieira, J. [4 ]
Fonseca, R. A. [4 ]
Silva, L. O. [4 ]
Gschwendtner, E. [3 ]
Muggli, P. [5 ]
机构
[1] Budker Inst Nucl Phys SB RAS, Novosibirsk 630090, Russia
[2] Novosibirsk State Univ, Novosibirsk 630090, Russia
[3] CERN, CH-1211 Geneva 23, Switzerland
[4] Univ Lisbon, Inst Super Tecn, Inst Plasmas & Fusao Nucl, P-1049001 Lisbon, Portugal
[5] Max Planck Inst Phys & Astrophys, D-80805 Munich, Germany
基金
俄罗斯科学基金会;
关键词
FACILITY; DYNAMICS;
D O I
10.1063/1.4904365
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
It is shown that co-linear injection of electrons or positrons into the wakefield of the self-modulating particle beam is possible and ensures high energy gain. The witness beam must copropagate with the tail part of the driver, since the plasma wave phase velocity there can exceed the light velocity, which is necessary for efficient acceleration. If the witness beam is many wakefield periods long, then the trapped charge is limited by beam loading effects. The initial trapping is better for positrons, but at the acceleration stage a considerable fraction of positrons is lost from the wave. For efficient trapping of electrons, the plasma boundary must be sharp, with the density transition region shorter than several centimeters. Positrons are not susceptible to the initial plasma density gradient. (C) 2014 AIP Publishing LLC.
引用
收藏
页数:8
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