scholarly journals Whistler wave radiation from a pulsed loop antenna located in a cylindrical duct with enhanced plasma density

2014 ◽  
Vol 21 (11) ◽  
pp. 112115 ◽  
Author(s):  
Alexander V. Kudrin ◽  
Natalya M. Shkokova ◽  
Orsolya E. Ferencz ◽  
Tatyana M. Zaboronkova
2002 ◽  
Vol 9 (4) ◽  
pp. 1401-1411 ◽  
Author(s):  
A. V. Kudrin ◽  
M. Yu. Lyakh ◽  
T. M. Zaboronkova ◽  
C. Krafft

2009 ◽  
Vol 16 (6) ◽  
pp. 063502 ◽  
Author(s):  
Alexander V. Kudrin ◽  
Pavel V. Bakharev ◽  
Catherine Krafft ◽  
Tatyana M. Zaboronkova

2007 ◽  
Vol 73 (6) ◽  
pp. 967-980
Author(s):  
C. KRAFFT ◽  
T. M. ZABORONKOVA

AbstractThe efficiency of whistler wave radiation by a density modulated and thin electron beam of finite length injected parallel with respect to the constant ambient magnetic field into a cylindrical plasma column surrounded by a uniform isotropic medium and aligned along the magnetic field is studied. A rigorous analytical derivation of the wave fields excited by the beam in the plasma column is presented. The time-averaged power radiated by the beam at the modulation frequency is determined. In particular, numerical calculations performed for physical conditions relevant to laboratory magnetized discharge plasmas show that, in the presence of a plasma column, the power lost by the modulated beam can be efficiently enhanced owing to resonant Cherenkov excitation of guided whistler modes at the beam modulation frequency.


2014 ◽  
Vol 81 (2) ◽  
Author(s):  
S. Saviz ◽  
S. Jafari

The theory for the two-stream free-electron laser with the whistler wave as a slow electromagnetic wave wiggler is studied theoretically. The results show that for small values of plasma density, there are seven groups of orbits and the plasma density enhancement leads to increase in the number of trajectories. Also, increasing the plasma density causes growth in the axial velocity for groups (1–4) of orbits and a reduction for groups (6–7). It is shown that for groups (6–7), the effect of plasma is to increase the gain, and for groups (1–4) the effect of plasma is to decrease the gain. For group (1) the effect of plasma is to decrease the maximum frequency and for group (3) it is to increase the maximum frequency.


2008 ◽  
Vol 77 (5) ◽  
pp. 055501 ◽  
Author(s):  
A V Kudrin ◽  
V A Es'kin ◽  
C Krafft ◽  
T M Zaboronkova

2008 ◽  
Vol 15 (7) ◽  
pp. 072114 ◽  
Author(s):  
Stephen Vincena ◽  
Walter Gekelman ◽  
M. A. Van Zeeland ◽  
James Maggs ◽  
Andrew Collette

2002 ◽  
Vol 8 (5-6) ◽  
pp. 96-101
Author(s):  
V.N. Fedun ◽  
◽  
A.K. Yukhimuk ◽  
A.D. Voitsekhovska ◽  
О.К. Cheremnykh ◽  
...  

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