scholarly journals Multi-angle multi-pulse time-resolved Thomson scattering on laboratory plasma jets

2018 ◽  
Vol 89 (10) ◽  
pp. 10C109 ◽  
Author(s):  
J. T. Banasek ◽  
S. V. R. Rocco ◽  
W. M. Potter ◽  
T. Byvank ◽  
B. R. Kusse ◽  
...  
2018 ◽  
Vol 46 (11) ◽  
pp. 3901-3905 ◽  
Author(s):  
J. T. Banasek ◽  
T. Byvank ◽  
S. V. R. Rocco ◽  
W. M. Potter ◽  
B. R. Kusse ◽  
...  

2020 ◽  
Vol 27 (6) ◽  
pp. 062708
Author(s):  
J. T. Banasek ◽  
S. V. R. Rocco ◽  
W. M. Potter ◽  
E. S. Lavine ◽  
B. R. Kusse ◽  
...  

2018 ◽  
Vol 6 ◽  
Author(s):  
A. Rigby ◽  
J. Katz ◽  
A. F. A. Bott ◽  
T. G. White ◽  
P. Tzeferacos ◽  
...  

Magnetic field measurements in turbulent plasmas are often difficult to perform. Here we show that for ${\geqslant}$kG magnetic fields, a time-resolved Faraday rotation measurement can be made at the OMEGA laser facility. This diagnostic has been implemented using the Thomson scattering probe beam and the resultant path-integrated magnetic field has been compared with that of proton radiography. Accurate measurement of magnetic fields is essential for satisfying the scientific goals of many current laser–plasma experiments.


2021 ◽  
Vol 28 (8) ◽  
pp. 082703
Author(s):  
J. T. Banasek ◽  
S. V. R. Rocco ◽  
W. M. Potter ◽  
E. S. Lavine ◽  
C. E. Seyler ◽  
...  

2020 ◽  
Vol 35 (9) ◽  
pp. 2064-2074
Author(s):  
Joost van der Mullen ◽  
Mariana Atanasova ◽  
Adam Obrusník ◽  
Lenka Zajíčková

This paper resolves a long standing discrepancy between theoretical modeling of atmospheric microwave plasma jets and their diagnostics by Thomson scattering. The discrepancy is found to be created by the filamentary behavior of the plasma.


2017 ◽  
Vol 24 (5) ◽  
pp. 054005 ◽  
Author(s):  
Simon Hübner ◽  
Joao Santos Sousa ◽  
Joost van der Mullen ◽  
William G Graham

2014 ◽  
Vol 81 (2) ◽  
Author(s):  
S. C. Hsu ◽  
A. L. Moser ◽  
E. C. Merritt ◽  
C. S. Adams ◽  
J. P. Dunn ◽  
...  

We describe a laboratory plasma physics experiment at Los Alamos National Laboratory that uses two merging supersonic plasma jets formed and launched by pulsed-power-driven railguns. The jets can be formed using any atomic species or mixture available in a compressed-gas bottle and have the following nominal initial parameters at the railgun nozzle exit: ne ≈ ni ~ 1016 cm−3, Te ≈ Ti ≈ 1.4 eV, Vjet ≈ 30–100 km/s, mean charge $\bar{Z}$ ≈ 1, sonic Mach number Ms ≡ Vjet/Cs > 10, jet diameter = 5 cm, and jet length ≈20 cm. Experiments to date have focused on the study of merging-jet dynamics and the shocks that form as a result of the interaction, in both collisional and collisionless regimes with respect to the inter-jet classical ion mean free path, and with and without an applied magnetic field. However, many other studies are also possible, as discussed in this paper.


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