Characterization of a compact gas-puff nozzle and plasma gun assembly for staged Z-pinch experiments

Author(s):  
F. Conti ◽  
J. C. Valenzuela ◽  
I. S. Krasheninnikov ◽  
V. A. Fadeev ◽  
J. Narkis ◽  
...  
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2012 ◽  
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pp. 034017 ◽  
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E Robert ◽  
V Sarron ◽  
D Riès ◽  
S Dozias ◽  
M Vandamme ◽  
...  

2001 ◽  
Vol 8 (5) ◽  
pp. 2257-2267 ◽  
Author(s):  
Michael E. Cuneo ◽  
Roger A. Vesey ◽  
John L. Porter ◽  
Gordon A. Chandler ◽  
David L. Fehl ◽  
...  

2007 ◽  
Vol 121-123 ◽  
pp. 885-888
Author(s):  
C.H. Zhang ◽  
S. Katsuki ◽  
J.G. Shi ◽  
H. Horita ◽  
T. Namihira ◽  
...  

In the development of our Z-pinch plasma EUV source, xenon (Xe) is used for the background gas discharges, and a solid tin (Sn) rod is used as target material due to its potential of high convention efficiency (CE) from input electric energy to EUV radiation [1, 2]. The Z-pinch plasma was driven by pulsed current with amplitude of 30 kA and pulse duration of 110 ns. Pinhole imaging, EUV spectrograph and in-band EUV energy monitor were used to characterize the EUV emission from the Z-pinch discharge. The experimental analyses have demonstrated the CE was as high as 3% [3].


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D G Fearn ◽  
E R Wooding
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1999 ◽  
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A. Lorenz ◽  
N. J. Peacock ◽  
M. G. O’Mullane ◽  
David Neely

2001 ◽  
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Author(s):  
T. W. L. Sanford ◽  
J. E. Bailey ◽  
G. A. Chandler ◽  
M. E. Cuneo ◽  
D. L. Fehl ◽  
...  
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X Rays ◽  

2016 ◽  
Vol 136 (3) ◽  
pp. 147-154 ◽  
Author(s):  
Ikko Sakuma ◽  
Yusuke Kikuchi ◽  
Wataru Isono ◽  
Takumi Nakazono ◽  
Masato Nakane ◽  
...  

2013 ◽  
Vol 55 (8) ◽  
pp. 085012 ◽  
Author(s):  
D Klir ◽  
A V Shishlov ◽  
V A Kokshenev ◽  
P Kubes ◽  
A Yu Labetsky ◽  
...  

2015 ◽  
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pp. 72001
Author(s):  
张庆军 Zhang Qingjun ◽  
方瑜 Fang Yu ◽  
罗炫 Luo Xuan ◽  
杨睿戆 Yang Ruizhuang ◽  
陈姝帆 Chen Shufan ◽  
...  

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