Modeling of secondary emission processes in the negative ion based electrostatic accelerator of the International Thermonuclear Experimental Reactor

The negative ion electrostatic accelerator for the neutral beam injector of the International Thermonuclear Experimental Reactor (ITER) is designed to deliver a negative deuterium current of 40 A at 1 MeV. Inside the accelerator there are several types of interactions that may create secondary parti...

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Main Authors: G. Fubiani, H. P. L. de Esch, A. Simonin, R. S. Hemsworth
Format: Article
Language:English
Published: American Physical Society 2008-01-01
Series:Physical Review Special Topics. Accelerators and Beams
Online Access:http://doi.org/10.1103/PhysRevSTAB.11.014202
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spelling doaj-231ef416d00d4274b54c170e2c0e29f02020-11-25T01:00:17ZengAmerican Physical SocietyPhysical Review Special Topics. Accelerators and Beams1098-44022008-01-0111101420210.1103/PhysRevSTAB.11.014202Modeling of secondary emission processes in the negative ion based electrostatic accelerator of the International Thermonuclear Experimental ReactorG. FubianiH. P. L. de EschA. SimoninR. S. HemsworthThe negative ion electrostatic accelerator for the neutral beam injector of the International Thermonuclear Experimental Reactor (ITER) is designed to deliver a negative deuterium current of 40 A at 1 MeV. Inside the accelerator there are several types of interactions that may create secondary particles. The dominating process originates from the single and double stripping of the accelerated negative ion by collision with the residual molecular deuterium gas (≃29% losses). The resulting secondary particles (positive ions, neutrals, and electrons) are accelerated and deflected by the electric and magnetic fields inside the accelerator and may induce more secondaries after a likely impact with the accelerator grids. This chain of reactions is responsible for a non-negligible heat load on the grids and must be understood in detail. In this paper, we will provide a comprehensive summary of the physics involved in the process of secondary emission in a typical ITER-like negative ion electrostatic accelerator together with a precise description of the numerical method and approximations involved. As an example, the multiaperture-multigrid accelerator concept will be discussed.http://doi.org/10.1103/PhysRevSTAB.11.014202
collection DOAJ
language English
format Article
sources DOAJ
author G. Fubiani
H. P. L. de Esch
A. Simonin
R. S. Hemsworth
spellingShingle G. Fubiani
H. P. L. de Esch
A. Simonin
R. S. Hemsworth
Modeling of secondary emission processes in the negative ion based electrostatic accelerator of the International Thermonuclear Experimental Reactor
Physical Review Special Topics. Accelerators and Beams
author_facet G. Fubiani
H. P. L. de Esch
A. Simonin
R. S. Hemsworth
author_sort G. Fubiani
title Modeling of secondary emission processes in the negative ion based electrostatic accelerator of the International Thermonuclear Experimental Reactor
title_short Modeling of secondary emission processes in the negative ion based electrostatic accelerator of the International Thermonuclear Experimental Reactor
title_full Modeling of secondary emission processes in the negative ion based electrostatic accelerator of the International Thermonuclear Experimental Reactor
title_fullStr Modeling of secondary emission processes in the negative ion based electrostatic accelerator of the International Thermonuclear Experimental Reactor
title_full_unstemmed Modeling of secondary emission processes in the negative ion based electrostatic accelerator of the International Thermonuclear Experimental Reactor
title_sort modeling of secondary emission processes in the negative ion based electrostatic accelerator of the international thermonuclear experimental reactor
publisher American Physical Society
series Physical Review Special Topics. Accelerators and Beams
issn 1098-4402
publishDate 2008-01-01
description The negative ion electrostatic accelerator for the neutral beam injector of the International Thermonuclear Experimental Reactor (ITER) is designed to deliver a negative deuterium current of 40 A at 1 MeV. Inside the accelerator there are several types of interactions that may create secondary particles. The dominating process originates from the single and double stripping of the accelerated negative ion by collision with the residual molecular deuterium gas (≃29% losses). The resulting secondary particles (positive ions, neutrals, and electrons) are accelerated and deflected by the electric and magnetic fields inside the accelerator and may induce more secondaries after a likely impact with the accelerator grids. This chain of reactions is responsible for a non-negligible heat load on the grids and must be understood in detail. In this paper, we will provide a comprehensive summary of the physics involved in the process of secondary emission in a typical ITER-like negative ion electrostatic accelerator together with a precise description of the numerical method and approximations involved. As an example, the multiaperture-multigrid accelerator concept will be discussed.
url http://doi.org/10.1103/PhysRevSTAB.11.014202
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