Plasma Parameters in the Reactor with Simultaneous Magnetron Discharge and Inductive Radio-Frequency Discharge in the Presence of External Magnetic Field

2018 ◽  
Vol 63 (4) ◽  
pp. 374-380 ◽  
Author(s):  
A. F. Aleksandrov ◽  
K. V. Vavilin ◽  
E. A. Kral’kina ◽  
P. A. Neklyudova ◽  
A. M. Nikonov ◽  
...  
2007 ◽  
Vol 40 (22) ◽  
pp. 7008-7018 ◽  
Author(s):  
J Schulze ◽  
T Gans ◽  
D O'Connell ◽  
U Czarnetzki ◽  
A R Ellingboe ◽  
...  

1992 ◽  
Vol 72 (7) ◽  
pp. 2632-2637 ◽  
Author(s):  
Jen‐Shih Chang ◽  
Y. Ichikawa ◽  
R. M. Hobson ◽  
S. Matsumura ◽  
S. Teii

Vacuum ◽  
2019 ◽  
Vol 169 ◽  
pp. 108927 ◽  
Author(s):  
A.K. Petrov ◽  
E.A. Kralkina ◽  
A.M. Nikonov ◽  
K.V. Vavilin ◽  
I.I. Zadiriev

Vacuum ◽  
2020 ◽  
Vol 181 ◽  
pp. 109634
Author(s):  
A.K. Petrov ◽  
E.A. Kralkina ◽  
A.M. Nikonov ◽  
K.V. Vavilin ◽  
I.I. Zadiriev

1975 ◽  
Vol 13 (2) ◽  
pp. 335-348 ◽  
Author(s):  
Chio-Zong Cheng

The instability of the ordinary electromagnetic mode, propagating perpendicular to an external magnetic field, is studied for a single-species plasma with ring velocity distribution. The marginal instability boundaries for both the purely growing mode and the propagating growing modes are calculated from the instability criteria. The dispersion characteristics for various sets of plasma parameters are also given. The frequency bands of the propagating growing modes are centered at about (η +½)ωc, where η = 1, 2,…, and the typical growth rates are of the order of the cyclotron frequency and enhanced by increasing fluβ1.


2021 ◽  
pp. 30-34
Author(s):  
О.V. Manuilenko ◽  
A.V. Pashchenko ◽  
V.G. Svichensky ◽  
B.V. Zajtsev

The analysis of the envelope equation for high-current relativistic electron beam propagation in plasma in an external uniform magnetic field is presented. The envelope equation is obtained in a Hamiltonian form with an effective potential, which depends from electron beam and plasma parameters, and external magnetic field. Hamiltonian aproach allows fully analyze the behavior of the beam envelope as a function of the beam current, beam energy, plasma density and conductivity, as well as on the external magnetic field and the initial beam angular momentum.


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