Study of negative hydrogen ion beam optics using the 2D PIC method

Author(s):  
K. Miyamoto ◽  
S. Okuda ◽  
A. Hatayama ◽  
M. Hanada ◽  
A. Kojima
2015 ◽  
Author(s):  
K. Miyamoto ◽  
S. Nishioka ◽  
I. Goto ◽  
A. Hatayama ◽  
M. Hanada ◽  
...  

2018 ◽  
Author(s):  
K. Miyamoto ◽  
S. Nishioka ◽  
A. Hatayama ◽  
T. Mizuno ◽  
J. Hiratsuka ◽  
...  

2016 ◽  
Vol 87 (2) ◽  
pp. 02B915 ◽  
Author(s):  
A. L. Zhang ◽  
S. X. Peng ◽  
H. T. Ren ◽  
T. Zhang ◽  
J. F. Zhang ◽  
...  

2015 ◽  
Vol 33 (2) ◽  
pp. 215-220 ◽  
Author(s):  
Ling-Yu Zhang ◽  
Xiao-Ying Zhao ◽  
Xin Qi ◽  
Guo-Qing Xiao ◽  
Wen-Shan Duan ◽  
...  

AbstractA two-dimensional particle-in-cell (PIC) simulation is carried out to study the wakefield and stopping power for a hydrogen ion beam pulse with low drift velocity propagation in hydrogen plasmas. The plasma is assumed to be collisionless, uniform, non-magnetized, and in a steady state. Both the pulse ions and plasma particles are treated by the PIC method. The effects of the beam density on the wakefield and stopping power are then obtained and discussed. It is found that as the beam densities increase, the oscillation wakefield induced by the beam become stronger. Besides, the first oscillation wakefield behind the bunch is particularly stronger than others. Moreover, it is found that the stationary stopping power increases linearly with the increase of the beam density in the linear/semilinear region.


2011 ◽  
Author(s):  
N. Miyamoto ◽  
M. Wada ◽  
Yasuhiko Takeiri ◽  
Katsuyoshi Tsumori

2011 ◽  
Author(s):  
Katsuhiro Shinto ◽  
Motoi Wada ◽  
Tomoaki Nishida ◽  
Yasuhiro Demura ◽  
Daichi Sasaki ◽  
...  

1985 ◽  
Vol 58 (7) ◽  
pp. 2492-2502 ◽  
Author(s):  
P. J. M. van Bommel ◽  
J. H. M. Bonnie ◽  
E. H. A. Granneman ◽  
P. Massmann ◽  
H. J. Hopman

2020 ◽  
Vol 1647 ◽  
pp. 012012
Author(s):  
R L Lapin ◽  
V A Skalyga ◽  
I V Izotov ◽  
S V Golubev ◽  
S V Razin ◽  
...  

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