2013
DOI: 10.1063/1.4824366
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Numerical study of atomic production rate in hydrogen negative ion sources with the effect of non-equilibrium electron energy distribution function

Abstract: Spatial non-uniformity of the dissociative hydrogen atom (H0) production has been investigated in a large negative ion source (JAEA 10 A source) with the electron energy distribution function (EEDF) obtained by a Monte-Carlo simulation code for electron transport in 3D3V (three dimensional real and velocity) space. It has been shown that the H0 production rate becomes larger in the upper region (one side in the longitudinal direction) of the source chamber. This spatial non-uniformity of the H0 production prof… Show more

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Cited by 23 publications
(21 citation statements)
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“…The detailed representations of the CR models for H and H 2 in non-equilibrium plasma (or EEDF) are shown in Ref. [4,5]. In the present model, Quasi-Steady State (QSS) assumption has been applied for excited molecules [6].…”
Section: -3mentioning
confidence: 99%
“…The detailed representations of the CR models for H and H 2 in non-equilibrium plasma (or EEDF) are shown in Ref. [4,5]. In the present model, Quasi-Steady State (QSS) assumption has been applied for excited molecules [6].…”
Section: -3mentioning
confidence: 99%
“…For example, such a kind of non-uniformity was observed in the N-NBI system [20] for the JAEA (Japan Atomic Energy Research Agency: * present QST: National Institute for Quantum and Radiological Science and Technology) JT-60U tokamak. The JT-60U tokamak is one of the largest magnetic fusion devices in the world and now is being upgraded to the JT-60SA with superconducting magnets for plasma confinement [24].A series of modeling studies [25][26][27][28][29][30][31] for such giant sources, more specifically, for the QST 10A source and JT-60SA H − source will be reviewed (section 2.3). The effect of the EEDFs on H − SP and the origin of H − beam non-uniformity will be discussed.…”
mentioning
confidence: 99%
“…In addition to the ground‐state atom modelled above, we solve a system of simultaneous rate equations for the population density of excited atoms with the quasi‐steady‐state collisional–radiative model (QSS‐CR) developed in refs . The QSS‐CR model can calculate H α intensity as well, and it enables our 0D model to simulate the experimental method for controlling the core plasma density in the QUEST tokamak.…”
Section: Model Equations For the Particle Balancementioning
confidence: 99%