EUV spectrometric facility with laser-focus plasma radiation source

1996 ◽  
Author(s):  
Valeri O. Papanyan ◽  
Gagik T. Nersisyan
2001 ◽  
Vol 19 (4) ◽  
pp. 579-595 ◽  
Author(s):  
D. MOSHER ◽  
B.V. WEBER ◽  
B. MOOSMAN ◽  
R.J. COMMISSO ◽  
P. COLEMAN ◽  
...  

High-sensitivity interferometry measurements of initial density distributions are reviewed for a wide range of gas-puff nozzles used in plasma radiation source (PRS) z-pinch experiments. Accurate gas distributions are required for determining experimental load parameters, modeling implosion dynamics, understanding the radiation properties of the stagnated pinch, and for predicting PRS performance in future experiments. For a number of these nozzles, a simple ballistic-gas-flow model (BFM) has been used to provide good physics-based analytic fits to the measured r, z density distributions. These BFM fits provide a convenient means to smoothly interpolate radial density distributions between discrete axial measurement locations for finer-zoned two-dimensional MHD calculations, and can be used to determine how changes in nozzle parameters and load geometry might alter implosion dynamics and radiation performance. These measurement and analysis techniques are demonstrated for a nested-shell nozzle used in Double Eagle and Saturn experiments. For this nozzle, the analysis suggests load modifications that may increase the K-shell yield.


1993 ◽  
Vol 23 (1) ◽  
pp. 76-80 ◽  
Author(s):  
I A Zhitnik ◽  
S V Kuzin ◽  
M M Mitropol'skiĭ ◽  
Evgenii N Ragozin ◽  
V A Slemzin ◽  
...  

2006 ◽  
Author(s):  
J. J. MacFarlane ◽  
P. Wang ◽  
I. E. Golovkin ◽  
P. R. Woodruff

2003 ◽  
Vol 21 (2) ◽  
pp. 255-264 ◽  
Author(s):  
S.A. CHAIKOVSKY ◽  
A.Yu. LABETSKY ◽  
V.I. ORESHKIN ◽  
A.V. SHISHLOV ◽  
R.B. BAKSHT ◽  
...  

A double shell z-pinch with an axial magnetic field is considered as a K-shell plasma radiation source. One-dimensional radiation-hydrodynamics calculations performed suggest that this scheme holds promise for the production of the K-shell radiation of krypton (hν ≈ 12–17 keV). As a first step in verifying the advantages of this scheme, experiments have been performed to optimize a neon double-shell gas puff with an axial magnetic yield for the K-shell yield and power. The experiments show that the application of an axial magnetic field makes it possible to increase the K-shell radiation power and reduce the shot-to-shot spread in the K-shell yield. Comparisons between the experiments and modeling are made and show good agreement.


1997 ◽  
Vol 81 (8) ◽  
pp. 3410-3415 ◽  
Author(s):  
F. J. Wessel ◽  
P. L. Coleman ◽  
N. Loter ◽  
P. Ney ◽  
H. U. Rahman ◽  
...  

2005 ◽  
Vol 78-79 ◽  
pp. 452-456 ◽  
Author(s):  
A. Bartnik ◽  
H. Fiedorowicz ◽  
R. Jarocki ◽  
L. Juha ◽  
J. Kostecki ◽  
...  

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