Discharge characteristics of bucket‐type ion source using a microwave plasma cathode

1990 ◽  
Vol 8 (3) ◽  
pp. 1831-1834 ◽  
Author(s):  
Y. Hakamata ◽  
T. Iga ◽  
Y. Ono ◽  
K. Natsui ◽  
T. Sato
1992 ◽  
Vol 63 (4) ◽  
pp. 2595-2597 ◽  
Author(s):  
Yoshio Matsubara ◽  
Hideaki Tahara ◽  
Masato Takahashi ◽  
Shuichi Nogawa ◽  
Junzo Ishikawa

1994 ◽  
Vol 65 (4) ◽  
pp. 1127-1128 ◽  
Author(s):  
Yusheng Rao ◽  
Jiannan Wu ◽  
Yuhong Yan ◽  
Yong Zhang ◽  
Lei Qi

1996 ◽  
Vol 67 (3) ◽  
pp. 1344-1346 ◽  
Author(s):  
G. Cojocaru ◽  
B. H. Wolf ◽  
H. Emig

Author(s):  
Yoshimi Hakamata ◽  
Takashi Iga ◽  
Ken'ichi Natsui ◽  
Tadashi Sato

1994 ◽  
Vol 65 (4) ◽  
pp. 1313-1315 ◽  
Author(s):  
Koji Miyake ◽  
Takashi Mikami ◽  
Hideaki Tahara ◽  
Kiyoshi Ogata ◽  
Yoshio Matsubara ◽  
...  

2004 ◽  
Vol 49 (1) ◽  
pp. 19-21
Author(s):  
N. V. Gavrilov ◽  
A. S. Kamenetskikh

1991 ◽  
Vol 30 (Part 2, No. 4B) ◽  
pp. L772-L774
Author(s):  
Genshiro Kawachi ◽  
Takashi Aoyama ◽  
Takaya Suzuki ◽  
Yasunori Ohno ◽  
Akio Mimura ◽  
...  

2005 ◽  
Vol 107 ◽  
pp. 21-24 ◽  
Author(s):  
M. Medhisuwakul ◽  
Thiraphat Vilaithong ◽  
Jürgen Engemann

A 13.56 MHz radio-frequency (rf) driven multicusp ion source has been constructed [1] to produce a high argon ion current density. Milliampere-range argon ion current can be extracted from the source. An in-waveguide microwave plasma source has been utilized as the ion beam neutralizer [2]. The neutralization source was placed 20 cm downstream from the extraction system. With the former extraction system, comprised of extraction electrodes and an Einzel lens, the electrons from the neutralizer were attracted to the high positive potential of the lens. Consequently, the potential of the lens drops and the beam is diverged. To suppress electrons from being accelerated to the Einzel lens a negatively biased electrode was placed before the last electrode, which is grounded, to produce a retarding electric field for electrons. The hole of the electrode was made small to make sure that the potential at the center is negative enough to suppress electrons. All simulations have been performed with the KOBRA3-INP simulation software. The results of the beam shape from the simulation will be presented.


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