1994
DOI: 10.1088/0022-3727/27/7/010
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Kinetics of metastable states in high-pressure nitrogen plasma pumped by high-current electron beam

Abstract: An effective method for calculating the electron energy distribution function in a plasma pumped by an electron beam is suggested. The electron impact excitation rates of different N2 and Hg states are obtained. The evolution of populations of the N2 excited states and of the Hg radiative states in a N2-Hg mixture is considered. The characteristic time tau e of equilibrium establishment is shown to be strongly dependent on the pressure of the mixture. The variation of the N2(A3 Sigma ) population is found to b… Show more

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Cited by 30 publications
(11 citation statements)
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“…For describing electron beam interaction with gas we used the results of [23,24], where it was shown that the rates of ionization, dissociation and excitation of different oxygen states by a high-energy electron beam could be written as:…”
Section: The Modelmentioning
confidence: 99%
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“…For describing electron beam interaction with gas we used the results of [23,24], where it was shown that the rates of ionization, dissociation and excitation of different oxygen states by a high-energy electron beam could be written as:…”
Section: The Modelmentioning
confidence: 99%
“…where E loss are electron energy losses on a unit of the length (depending on the electron energy), j b is the beam current density and U k are the energy costs of the corresponding loss processes [23,24]. The kinetic model for argon-oxygen mixtures included the basic kinds of charged and neutral particles: electrons, negative ions, positive ions (both oxygen and argon), oxygen molecules in the ground-O 2 (X…”
Section: The Modelmentioning
confidence: 99%
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“…For example, additional population by vibrational relaxation of N 2 (C 3 Π u , v > 0) states recently suggested by [4] is not relevant at the conditions of present work: the time of vibrational relaxation of N 2 (C 3 Π u , v = 1, 2) is about 110-120 ns. It should also be noted that the main population of N 2 (C 3 Π u ) in the discharge afterglow occurs in the self-quenching reaction of N 2 (A 3 Σ + u ) molecules and during the electron-ion recombination N + 4 + e → N 2 (C 3 Π u ) + N 2 [49]. The decay of a given electronic state, in case of low specific deposited energy discharges at moderate pressure, is determined by the radiative decay and by the quenching by background gas only.…”
Section: Discussionmentioning
confidence: 99%
“…Determination of the concentration of N 2 (A 3 Σ u + ) by combining emission spectroscopy measurements with modeling of the generation and decay of excited molecules, atoms, and ions has also been reported [16,17]. Modeling based on pure calculations without using optical emission data has also been performed [18][19][20], but these focus on the low-pressure regions commonly used in plasma processes.…”
Section: Examples Of N2(mentioning
confidence: 99%