Influence of Discharge Plasma Inhomogeneities on the Characteristics of KrF-Laser Radiation

2021 ◽  
Vol 63 (12) ◽  
pp. 2070-2075
Author(s):  
Hongda Li ◽  
Y. N. Panchenko ◽  
M. V. Andreev ◽  
A. V. Puchikin ◽  
S. A. Yampolskaya ◽  
...  
1983 ◽  
Vol 44 (C2) ◽  
pp. C2-19-C2-25
Author(s):  
M. C. Gower ◽  
R. G. Caro

1993 ◽  
Vol 14 (6) ◽  
pp. 421-425 ◽  
Author(s):  
V. S. Barabanov ◽  
V. L. Kantsyrev ◽  
N. V. Morozov ◽  
P. B. Sergeev ◽  
M. A. Tyunina

1989 ◽  
Vol 28 (10) ◽  
pp. 1877 ◽  
Author(s):  
Robert Fedosejevs ◽  
M. J. Brett

1984 ◽  
Vol 14 (7) ◽  
pp. 937-939
Author(s):  
A D Klementov ◽  
Nikolai V Morozov ◽  
P B Sergeev

2019 ◽  
Vol 49 (12) ◽  
pp. 1112-1116
Author(s):  
O N Egorova ◽  
O I Medvedkov ◽  
E S Seregin ◽  
S A Vasil'ev ◽  
S E Sverchkov ◽  
...  

10.14311/1123 ◽  
2009 ◽  
Vol 49 (2) ◽  
Author(s):  
M. Nevrkla

A device producing Z-pinching plasma as a source of XUV radiation is described. Here a ceramic capacitor bank pulse-charged up to 100 kV is discharged through a pre-ionized gas-filled ceramic tube 3.2 mm in diameter and 21 cm in length. The discharge current has amplitude of 20 kA and a rise-time of 65 ns. The apparatus will serve as experimental device for studying of capillary discharge plasma, for testing X-ray optics elements and for investigating the interaction of water-window radiation with biological samples. After optimization it will be able to produce 46.9 nm laser radiation with collision pumped Ne-like argon ions active medium. 


1994 ◽  
Author(s):  
A. A. Offenberger ◽  
W. Blyth ◽  
A. E. Dangor ◽  
A. Djaoui ◽  
M. H. Key ◽  
...  
Keyword(s):  

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