Ion Cyclotron Drift Waves in Plasmas with Controlled Radial Density Distributions

1987 ◽  
Vol 26 (Part 1, No. 3) ◽  
pp. 444-450
Author(s):  
Masashi Kando ◽  
Shunjiro Ikezawa ◽  
Hideo Sugai ◽  
Shigeru Kishimoto
1988 ◽  
Vol 27 (Part 1, No. 11) ◽  
pp. 2128-2133
Author(s):  
Masashi Kando ◽  
Shigeru Kishimoto ◽  
Hideo Sugai ◽  
Shunjiro Ikezawa

1969 ◽  
Vol 47 (12) ◽  
pp. 2306-2307 ◽  
Author(s):  
N. C. Baird

Molecular orbital calculations by the MINDO method are reported for the valence electrons of HO− and a number of small alkoxide anions. The acidity order [Formula: see text] is predicted, in agreement with recent ion cyclotron resonance studies. The electron density distributions within the ions are discussed with reference to current models of the polarizability of alkyl groups.


1980 ◽  
Vol 240 ◽  
pp. 74 ◽  
Author(s):  
L. H. Cheung ◽  
J. A. Frogel ◽  
M. G. Hauser ◽  
D. Y. Gezari

1996 ◽  
Vol 56 (1) ◽  
pp. 187-191 ◽  
Author(s):  
O. A. Pokhotelov ◽  
L. Stenflo ◽  
P. K. Shukla

Model equations describing the nonlinear coupling between electrostatic ion-cyclotron and drift waves are derived, taking into account the action of the low-frequency ponderomotive force associated with the ion-cyclotron waves. It is found that this interaction is governed by a pair of equations, which can be used for studying the modulational instability of a constant amplitude ion-cyclotron wave as well as the dynamics of nonlinearly coupled ion-cyclotron and drift waves.


2001 ◽  
Vol 63 (18) ◽  
Author(s):  
Jan Harms ◽  
J. Peter Toennies ◽  
Manuel Barranco ◽  
Marti Pi

1999 ◽  
Vol 52 (1) ◽  
pp. 59
Author(s):  
J. L. V. Lewandowski

The radial structure of electron drift waves in a low-pressure tokamak plasma is presented. The ions are cold and an electrostatic approximation for the fluctuating potential is used. It is shown that problem of the radial structure of drift waves in toroidal geometry is amenable to a two-step solution; in the first approximation, the radial structure of the mode is neglected and the problem to be solved is the usual eigenmode equation along the (extended) poloidal angle; in the second approximation, the mode amplitude is expanded in ascending powers of the parameter (k⊥Ln)–1/2, where k⊥ is the magnitude of the lowest-order wavevector and Ln is the radial density scalelength. The implications of these radially-extended drift-type modes for the anomalous cross-field diffusion are discussed.


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