Dissociative recombination and electron-impact de-excitation in CH photon emission under ITER divertor-relevant plasma conditions

被引:15
作者
van Swaaij, G. A. [1 ]
Bystrov, K. [1 ]
Borodin, D. [2 ]
Kirschner, A. [2 ]
van der Vegt, L. B. [1 ]
van Rooij, G. J. [1 ]
De Temmerman, G. [1 ]
Goedheer, W. J. [1 ]
机构
[1] EURATOM, FOM Inst DIFFER, NL-3430 BE Nieuwegein, Netherlands
[2] Assoc EURATOM FZJ, Forschungszentrum Julich GmbH, Inst Energy & Climate Res Plasma Phys, D-52425 Julich, Germany
关键词
CHEMICAL EROSION; HYDROCARBON INJECTION; LOW-TEMPERATURE; SPECTROSCOPY; SIMULATION; LIFETIME; RADICALS; TOKAMAKS; FLUX;
D O I
10.1088/0741-3335/54/9/095013
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
For understanding carbon erosion and redeposition in nuclear fusion devices, it is important to understand the transport and chemical break-up of hydrocarbon molecules in edge plasmas, often diagnosed by emission of the CH A(2)Delta-X-2 Pi Gero band around 430 nm. The CH A-level can be excited either by electron-impact (EI) or by dissociative recombination (DR) of hydrocarbon ions. These processes were included in the 3D Monte Carlo impurity transport code ERO. A series of methane injection experiments was performed in the high-density, low-temperature linear plasma generator Pilot-PSI, and simulated emission intensity profiles were benchmarked against these experiments. It was confirmed that excitation by DR dominates at T-e < 1.5 eV. The results indicate that the fraction of DR events that lead to a CH radical in the A-level and consequent photon emission is at least 10%. Additionally, quenching of the excited CH radicals by EI de-excitation was included in the modeling. This quenching is shown to be significant: depending on the electron density, it reduces the effective CH emission by a factor of 1.4 at n(e) = 1.3 x 10(20) m(-3), to 2.8 at n(e) = 9.3 x 10(20) m(-3). Its inclusion significantly improved agreement between experiment and modeling.
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页数:9
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