scholarly journals Conditions for soft x-ray lasing action in a confined plasma column

1979 ◽  
Author(s):  
S. Suckewer ◽  
H. Fishman
Keyword(s):  
1980 ◽  
Vol 51 (4) ◽  
pp. 1922 ◽  
Author(s):  
S. Suckewer ◽  
H. Fishman
Keyword(s):  

1986 ◽  
Author(s):  
S. Suckewer ◽  
C. H. Skinner ◽  
C. Keane ◽  
D. Kim ◽  
J. L. Schwob ◽  
...  
Keyword(s):  

1985 ◽  
Vol 55 (17) ◽  
pp. 1753-1756 ◽  
Author(s):  
S. Suckewer ◽  
C. H. Skinner ◽  
H. Milchberg ◽  
C. Keane ◽  
D. Voorhees
Keyword(s):  

1983 ◽  
Vol 19 (12) ◽  
pp. 1855-1860 ◽  
Author(s):  
S. Suckewer ◽  
C. Skinner ◽  
D. Voorhees ◽  
H. Milchberg ◽  
C. Keane ◽  
...  

1992 ◽  
Vol 10 (4) ◽  
pp. 767-776 ◽  
Author(s):  
T. Pisarczyk ◽  
A. Faryński ◽  
H. Fiedorowicz ◽  
P. Gogolewski ◽  
M. Kuśnierz ◽  
...  

In this article, we present the formation of an elongated plasma column by combining a laser plasma with an external magnetic field. The laser plasma is produced by irradiating solid targets with a focused Nd-glass laser. The targets were placed on the axis of the two, single-turn magnetic coils, which provided a magnetic field up to 500 kg in the target region. The expanding laser plasma is confined by the magnetic field and an elongated and uniform plasma column is formed on the axis of the coils. The plasma column emits strong, soft X-ray radiation. The pinhole photographs show that the plasma column is at least 5 mm long. To study the interaction of the expanding laser plasma with a magnetic field, the laser probing diagnostic was used.


1985 ◽  
Author(s):  
S. Suckewer ◽  
C.H. Skinner ◽  
H. Milchberg ◽  
C. Keane ◽  
D. Voorhees
Keyword(s):  
X Ray ◽  

10.14311/1755 ◽  
2013 ◽  
Vol 53 (2) ◽  
Author(s):  
Jiri Kortanek ◽  
Pavel Kubes

Processed data is taken from the D-D fusion reaction experiments on PF-1000 at IFPILM Warsaw, operating with 2 MA, 1011 neutron yield, using interferometry, temporal resolved neutron diagnostics, magnetic probe diagnostics and X-ray diagnostics. The inductance is calculated under two different circumstances: with the known distribution function determined by the magnetic probe signal, and with the border of the plasma column determined from interferograms using Matlab. The inductance of the whole column is calculated using the formula for the inductance of a coaxial cylinder.


1988 ◽  
Vol 7 (4) ◽  
pp. 337-342 ◽  
Author(s):  
P Jaegle ◽  
A Carillon ◽  
P Dhez ◽  
B Gauthe ◽  
F Gadi ◽  
...  
Keyword(s):  
X Ray ◽  

1983 ◽  
Author(s):  
S. Suckewer ◽  
C.H. Skinner ◽  
D. Voorhees ◽  
H. Milchberg ◽  
C. Keane ◽  
...  

1996 ◽  
Vol 14 (2) ◽  
pp. 253-260 ◽  
Author(s):  
Henryk Fiedorowicz ◽  
Andrzej Bartnik ◽  
Mirosław Szczurek ◽  
Ernst Fill ◽  
Yuelin Li ◽  
...  

We report the first studies on the formation of an elongated plasma column suitable for X-ray laser experiments, using a gas puff target irradiated with a high-power laser. The gas puff targets, produced by pulsed injection of a small amount of gas from a high-pressure solenoid valve through a nozzle in the form of a slit, have been characterized by optical interferometry and X-ray backlighting. The formation of a hot plasma column up to 30-mm-long is demonstrated. The spatial uniformity of the column was monitored by means of an X-ray pinhole camera. XUV spectra measurements for SF6 gas puff targets show predominant 3–2 line of hydrogenic fluorine (λ = 8.1 nm), however, only linear increasing of its intensity with the target length was observed.


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