New high-frequency effect due to the drift velocity of a plasma: A plasma HF analog of the Roentgen-Eichenwald current

A. M. Messiaen; P. E. Vandenplas

doi:10.1016/0031-9163(66)91027-4

New high-frequency effect due to the drift velocity of a plasma: A plasma HF analog of the Roentgen-Eichenwald current

A. M. Messiaen, P. E. Vandenplas

Laboratory for Plasma Physics

California Institute of Technology

Research output: Contribution to journal › Article › peer-review

Abstract

The axial drift velocity v_d of a plasma column couples the transverse electric field E_c of an incoming wave to a scattered axial field E_Zsc. Both the position and the angular dependence, but not the magnitude, of the resonances of E_Zsc (including the complication introduced by a steady axial magnetic field) are very well explained by a cold plasma model.

Original language	English
Pages (from-to)	14-15
Number of pages	2
Journal	Physics Letters
Volume	20
Issue number	1
DOIs	https://doi.org/10.1016/0031-9163(66)91027-4
Publication status	Published - 15 Jan 1966

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title = "New high-frequency effect due to the drift velocity of a plasma: A plasma HF analog of the Roentgen-Eichenwald current",

abstract = "The axial drift velocity vd of a plasma column couples the transverse electric field Ec of an incoming wave to a scattered axial field EZsc. Both the position and the angular dependence, but not the magnitude, of the resonances of EZsc (including the complication introduced by a steady axial magnetic field) are very well explained by a cold plasma model.",

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T2 - A plasma HF analog of the Roentgen-Eichenwald current

AU - Messiaen, A. M.

AU - Vandenplas, P. E.

PY - 1966/1/15

Y1 - 1966/1/15

N2 - The axial drift velocity vd of a plasma column couples the transverse electric field Ec of an incoming wave to a scattered axial field EZsc. Both the position and the angular dependence, but not the magnitude, of the resonances of EZsc (including the complication introduced by a steady axial magnetic field) are very well explained by a cold plasma model.

AB - The axial drift velocity vd of a plasma column couples the transverse electric field Ec of an incoming wave to a scattered axial field EZsc. Both the position and the angular dependence, but not the magnitude, of the resonances of EZsc (including the complication introduced by a steady axial magnetic field) are very well explained by a cold plasma model.

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New high-frequency effect due to the drift velocity of a plasma: A plasma HF analog of the Roentgen-Eichenwald current

Abstract

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