Resonant-to-nonresonant transition in electrostatic ion-cyclotron wave phase velocity
Because of the implications for plasmas in the laboratory and in space, attention has been drawn to inhomogeneous energy-density driven (IEDD) waves that are sustained by velocity-shear-induced inhomogeneity in cross-field plasma flow. These waves have a frequency <font face='Symbol'...
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doaj-87e50b63a41140c684ace42011b4e0df2020-11-25T00:52:26ZengCopernicus PublicationsNonlinear Processes in Geophysics1023-58091607-79462003-01-01101/2131138Resonant-to-nonresonant transition in electrostatic ion-cyclotron wave phase velocityJ. J. Carroll IIIJ. J. Carroll IIIM. E. KoepkeM. W. ZintlM. W. ZintlV. GavrishchakaBecause of the implications for plasmas in the laboratory and in space, attention has been drawn to inhomogeneous energy-density driven (IEDD) waves that are sustained by velocity-shear-induced inhomogeneity in cross-field plasma flow. These waves have a frequency <font face='Symbol'>v</font><sub>r</sub> in the lab frame within an order of magnitude of the ion gyrofrequency <font face='Symbol'>v</font><sub>ci</sub>, propagate nearly perpendicular to the magnetic field (k<sub>z</sub> /k<font face='Symbol'><sub>^</sub></font> << 1), and can be Landau resonant (0 < <font face='Symbol'>v</font><sub>1</sub>/k<sub>z</sub> < <font face='Symbol'>n</font><sub>d</sub>) with a parallel drifting electron population (drift speed <font face='Symbol'>n</font><sub>d</sub>), where subscripts <i>1</i> and <i>r</i> indicate frequency in the frame of flowing ions and in the lab frame, respectively, and k<sub>z</sub> is the parallel component of the wavevector. A transition in phase velocity from 0 < <font face='Symbol'>v</font><sub>1</sub>/k<sub>z</sub> < <font face='Symbol'>n</font><sub>d</sub> to 0 > <font face='Symbol'>v</font><sub>1</sub>/k<sub>z</sub> > <font face='Symbol'>n</font><sub>d</sub> for a pair of IEDD eigenmodes is observed as the degree of in-homogeneity in the transverse <b><i>E × B</i></b> flow is increased in a magnetized plasma column. For weaker velocity shear, both eigenmodes are dissipative, i.e. in Landau resonance, with k<sub>z</sub> <font face='Symbol'>n</font><sub>d</sub> > 0. For stronger shear, both eigenmodes become reactive, with one's wavevector component k<sub>z</sub> remaining parallel, but with <font face='Symbol'>v</font><sub>1</sub>/k<sub>z</sub> > <font face='Symbol'>n</font><sub>d</sub> , and the other's wavevector component k<sub>z</sub> becoming anti-parallel, so that 0 > <font face='Symbol'>v</font><sub>1</sub>/k<sub>z</sub> . For both eigenmodes, the transition (1) involves a small frequency shift and (2) does not involve a sign change in the wave energy density, which is proportional to <font face='Symbol'>v</font><sub>r</sub> <font face='Symbol'>v</font><sub>1</sub>, both of which are previously unrecognized aspects of inhomogeneous energy-density driven waves.http://www.nonlin-processes-geophys.net/10/131/2003/npg-10-131-2003.pdf |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
J. J. Carroll III J. J. Carroll III M. E. Koepke M. W. Zintl M. W. Zintl V. Gavrishchaka |
spellingShingle |
J. J. Carroll III J. J. Carroll III M. E. Koepke M. W. Zintl M. W. Zintl V. Gavrishchaka Resonant-to-nonresonant transition in electrostatic ion-cyclotron wave phase velocity Nonlinear Processes in Geophysics |
author_facet |
J. J. Carroll III J. J. Carroll III M. E. Koepke M. W. Zintl M. W. Zintl V. Gavrishchaka |
author_sort |
J. J. Carroll III |
title |
Resonant-to-nonresonant transition in electrostatic ion-cyclotron wave phase velocity |
title_short |
Resonant-to-nonresonant transition in electrostatic ion-cyclotron wave phase velocity |
title_full |
Resonant-to-nonresonant transition in electrostatic ion-cyclotron wave phase velocity |
title_fullStr |
Resonant-to-nonresonant transition in electrostatic ion-cyclotron wave phase velocity |
title_full_unstemmed |
Resonant-to-nonresonant transition in electrostatic ion-cyclotron wave phase velocity |
title_sort |
resonant-to-nonresonant transition in electrostatic ion-cyclotron wave phase velocity |
publisher |
Copernicus Publications |
series |
Nonlinear Processes in Geophysics |
issn |
1023-5809 1607-7946 |
publishDate |
2003-01-01 |
description |
Because of the implications for plasmas in the laboratory and in space, attention has been drawn to inhomogeneous energy-density driven (IEDD) waves that are sustained by velocity-shear-induced inhomogeneity in cross-field plasma flow. These waves have a frequency <font face='Symbol'>v</font><sub>r</sub> in the lab frame within an order of magnitude of the ion gyrofrequency <font face='Symbol'>v</font><sub>ci</sub>, propagate nearly perpendicular to the magnetic field (k<sub>z</sub> /k<font face='Symbol'><sub>^</sub></font> << 1), and can be Landau resonant (0 < <font face='Symbol'>v</font><sub>1</sub>/k<sub>z</sub> < <font face='Symbol'>n</font><sub>d</sub>) with a parallel drifting electron population (drift speed <font face='Symbol'>n</font><sub>d</sub>), where subscripts <i>1</i> and <i>r</i> indicate frequency in the frame of flowing ions and in the lab frame, respectively, and k<sub>z</sub> is the parallel component of the wavevector. A transition in phase velocity from 0 < <font face='Symbol'>v</font><sub>1</sub>/k<sub>z</sub> < <font face='Symbol'>n</font><sub>d</sub> to 0 > <font face='Symbol'>v</font><sub>1</sub>/k<sub>z</sub> > <font face='Symbol'>n</font><sub>d</sub> for a pair of IEDD eigenmodes is observed as the degree of in-homogeneity in the transverse <b><i>E × B</i></b> flow is increased in a magnetized plasma column. For weaker velocity shear, both eigenmodes are dissipative, i.e. in Landau resonance, with k<sub>z</sub> <font face='Symbol'>n</font><sub>d</sub> > 0. For stronger shear, both eigenmodes become reactive, with one's wavevector component k<sub>z</sub> remaining parallel, but with <font face='Symbol'>v</font><sub>1</sub>/k<sub>z</sub> > <font face='Symbol'>n</font><sub>d</sub> , and the other's wavevector component k<sub>z</sub> becoming anti-parallel, so that 0 > <font face='Symbol'>v</font><sub>1</sub>/k<sub>z</sub> . For both eigenmodes, the transition (1) involves a small frequency shift and (2) does not involve a sign change in the wave energy density, which is proportional to <font face='Symbol'>v</font><sub>r</sub> <font face='Symbol'>v</font><sub>1</sub>, both of which are previously unrecognized aspects of inhomogeneous energy-density driven waves. |
url |
http://www.nonlin-processes-geophys.net/10/131/2003/npg-10-131-2003.pdf |
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