TY - JOUR
T1 - Dissociative recombination and electron-impact de-excitation in CH photon emission under ITER divertor-relevant plasma conditions
AU - Van Swaaij, G. A.
AU - Bystrov, K.
AU - Borodin, D.
AU - Kirschner, A.
AU - Van Der Vegt, L. B.
AU - Van Rooij, G. J.
AU - De Temmerman, G.
AU - Goedheer, W. J.
PY - 2012/9
Y1 - 2012/9
N2 - 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 2Δ-X 2Π Gerö band around 430nm. 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<1.5eV. 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=1.3×10 20m 3, to 2.8 at n e=9.3×10 20m 3. Its inclusion significantly improved agreement between experiment and modeling.
AB - 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 2Δ-X 2Π Gerö band around 430nm. 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<1.5eV. 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=1.3×10 20m 3, to 2.8 at n e=9.3×10 20m 3. Its inclusion significantly improved agreement between experiment and modeling.
UR - http://www.scopus.com/inward/record.url?scp=84865188039&partnerID=8YFLogxK
U2 - 10.1088/0741-3335/54/9/095013
DO - 10.1088/0741-3335/54/9/095013
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AN - SCOPUS:84865188039
SN - 0741-3335
VL - 54
JO - Plasma Physics and Controlled Fusion
JF - Plasma Physics and Controlled Fusion
IS - 9
M1 - 095013
ER -