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Title: Role of electrostatic and magnetic electron confinement in a hollow-cathode glow discharge in a nonuniform magnetic field

Abstract

Glow discharge with electron confinement in an electrostatic trap has been studied. The trap is formed by a cylindrical hollow cathode, as well as by a flat target on its bottom and a grid covering its output aperture, both being negatively biased relative to the cathode. At a gas pressure of 0.2–0.4 Pa, the fraction of ions sputtering the target (δ = 0.13) in the entire number of ions emitted by the uniform discharge plasma corresponds to the ratio of the target surface area to the total surface area of the cathode, grid, and target. When a nonuniform magnetic field with force lines passing through the target center (where the magnetic induction reaches 35 mT), as well as through the grid, hollow cathode, and target periphery (where the field lines are arc-shaped), is applied to the trap, its influence on the discharge depends on the magnetic induction B{sub 0} at the target edge. At B{sub 0} = 1 mT, the electrons emitted from the target periphery and drifting azimuthally in the arc-shaped field insignificantly contribute to gas ionization. Nevertheless, since fast electrons that are emitted from the cathode and oscillate inside it are forced by the magnetic field to comemore » more frequently to the target, thereby intensifying gas ionization near the latter, the fraction δ doubles and the plasma density near the target becomes more than twice as high as that near the grid. At B{sub 0} = 6 mT, the contribution of electrons emitted from the target surface to gas ionization near the target grows up and δ increases two more times. At cathode-target voltages in the range of 0–3 kV, the current in the target circuit vanishes as the voltage between the anode and the cathode decreases to zero.« less

Authors:
; ; ; ;  [1]
  1. Moscow State University of Technology “STANKIN,” (Russian Federation)
Publication Date:
OSTI Identifier:
22472444
Resource Type:
Journal Article
Resource Relation:
Journal Name: Plasma Physics Reports; Journal Volume: 41; Journal Issue: 2; Other Information: Copyright (c) 2015 Pleiades Publishing, Ltd.; Country of input: International Atomic Energy Agency (IAEA)
Country of Publication:
United States
Language:
English
Subject:
70 PLASMA PHYSICS AND FUSION TECHNOLOGY; ANODES; ELECTRIC CURRENTS; ELECTRIC POTENTIAL; ELECTRONS; EMISSION; GLOW DISCHARGES; HOLLOW CATHODES; INDUCTION; MAGNETIC CONFINEMENT; MAGNETIC FIELDS; PLASMA DENSITY; TRAPS

Citation Formats

Metel, A. S., E-mail: a.metel@stankin.ru, Grigoriev, S. N., Volosova, M. A., Bolbukov, V. P., and Melnik, Yu. A. Role of electrostatic and magnetic electron confinement in a hollow-cathode glow discharge in a nonuniform magnetic field. United States: N. p., 2015. Web. doi:10.1134/S1063780X14120058.
Metel, A. S., E-mail: a.metel@stankin.ru, Grigoriev, S. N., Volosova, M. A., Bolbukov, V. P., & Melnik, Yu. A. Role of electrostatic and magnetic electron confinement in a hollow-cathode glow discharge in a nonuniform magnetic field. United States. doi:10.1134/S1063780X14120058.
Metel, A. S., E-mail: a.metel@stankin.ru, Grigoriev, S. N., Volosova, M. A., Bolbukov, V. P., and Melnik, Yu. A. Sun . "Role of electrostatic and magnetic electron confinement in a hollow-cathode glow discharge in a nonuniform magnetic field". United States. doi:10.1134/S1063780X14120058.
@article{osti_22472444,
title = {Role of electrostatic and magnetic electron confinement in a hollow-cathode glow discharge in a nonuniform magnetic field},
author = {Metel, A. S., E-mail: a.metel@stankin.ru and Grigoriev, S. N. and Volosova, M. A. and Bolbukov, V. P. and Melnik, Yu. A.},
abstractNote = {Glow discharge with electron confinement in an electrostatic trap has been studied. The trap is formed by a cylindrical hollow cathode, as well as by a flat target on its bottom and a grid covering its output aperture, both being negatively biased relative to the cathode. At a gas pressure of 0.2–0.4 Pa, the fraction of ions sputtering the target (δ = 0.13) in the entire number of ions emitted by the uniform discharge plasma corresponds to the ratio of the target surface area to the total surface area of the cathode, grid, and target. When a nonuniform magnetic field with force lines passing through the target center (where the magnetic induction reaches 35 mT), as well as through the grid, hollow cathode, and target periphery (where the field lines are arc-shaped), is applied to the trap, its influence on the discharge depends on the magnetic induction B{sub 0} at the target edge. At B{sub 0} = 1 mT, the electrons emitted from the target periphery and drifting azimuthally in the arc-shaped field insignificantly contribute to gas ionization. Nevertheless, since fast electrons that are emitted from the cathode and oscillate inside it are forced by the magnetic field to come more frequently to the target, thereby intensifying gas ionization near the latter, the fraction δ doubles and the plasma density near the target becomes more than twice as high as that near the grid. At B{sub 0} = 6 mT, the contribution of electrons emitted from the target surface to gas ionization near the target grows up and δ increases two more times. At cathode-target voltages in the range of 0–3 kV, the current in the target circuit vanishes as the voltage between the anode and the cathode decreases to zero.},
doi = {10.1134/S1063780X14120058},
journal = {Plasma Physics Reports},
number = 2,
volume = 41,
place = {United States},
year = {Sun Feb 15 00:00:00 EST 2015},
month = {Sun Feb 15 00:00:00 EST 2015}
}