The temporal evolution of a potential double layer formed by ion beam reflection in a magnetized plasma

1985 ◽  
Vol 28 (2) ◽  
pp. 712 ◽  
Author(s):  
H. Fujita ◽  
S. Yagura
1982 ◽  
Vol 24 (11) ◽  
pp. 1465-1473 ◽  
Author(s):  
S Yagura ◽  
H Fujita ◽  
E Yamada

2021 ◽  
Vol 0 (0) ◽  
Author(s):  
Debdatta Debnath ◽  
Anup Bandyopadhyay

Abstract At the acoustic speed, we have investigated the existence of ion-acoustic solitary structures including double layers and supersolitons in a collisionless magnetized plasma consisting of negatively charged static dust grains, adiabatic warm ions, and nonthermal electrons. At the acoustic speed, for negative polarity, the system supports solitons, double layers, supersoliton structures after the formation of double layer, supersoliton structures without the formation of double layer, solitons after the formation of double layer whereas the system supports solitons and supersolitons without the formation of double layer for the case of positive polarity. But it is not possible to get the coexistence of solitary structures (including double layers and supersolitons) of opposite polarities. For negative polarity, we have observed an important transformation viz., soliton before the formation of double layer → double layer → supersoliton → soliton after the formation of double layer whereas for both positive and negative polarities, we have observed the transformation from solitons to supersolitons without the formation of double layer. There does not exist any negative (positive) potential solitary structures within 0 < μ < μ c (μ c < μ < 1) and the amplitude of the positive (negative) potential solitary structure decreases for increasing (decreasing) μ and the solitary structures of both polarities collapse at μ = μ c, where μ c is a critical value of μ, the ratio of the unperturbed number density of electrons to that of ions. Similarly there exists a critical value β e2 of the nonthermal parameter β e such that the solitons of both polarities collapse at β e = β e2.


1998 ◽  
Vol 38 (5) ◽  
pp. 661-671 ◽  
Author(s):  
E.V Suvorov ◽  
E Holzhauer ◽  
W Kasparek ◽  
A.B Burov ◽  
Y.A Dryagin ◽  
...  

2010 ◽  
Vol 81 (2) ◽  
pp. 02B310
Author(s):  
S. Imakita ◽  
N. Miyamoto ◽  
T. Kasuya ◽  
Y. Kimura ◽  
M. Wada

2014 ◽  
Vol 53 (5S1) ◽  
pp. 05FB10 ◽  
Author(s):  
Akira Okada ◽  
Kenichi Uehara ◽  
Miyoshi Yokura ◽  
Masahito Matsui ◽  
Katsuhiko Inaba ◽  
...  

1976 ◽  
Vol 16 (2) ◽  
pp. 149-169 ◽  
Author(s):  
John D. Gaffey

The Fokker-Planck equation is studied for an energetic ion beam injected into a magnetized plasma consisting of Maxwellian ions and electrons with υthi ≪υb≪ υthe. The time evolution of the fast ion distribution is given in terms of an infinite sum of Legendre polynomials for distributions that are axisymmetric about the magnetic field. The effect of charge exchange is included. The resulting ion distribution is somewhat isotropic for velocities much less than the injection velocity, however, the distribution is sharply peaked in both energy and pitch angle for velocities near the injection velocity. Approximate asymptotic expressions are given for the distribution in the vicinity of the injected beam and for velocities greater than the injection velocity. The effect of a weak parallel electric field is also given.


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