TY - JOUR
T1 - Edge and core impurity transport study with spectroscopic instruments in LHD
AU - Morita, Shigeru
AU - Goto, Motoshi
AU - Kobayashi, Masahiro
AU - Muto, Sadatsugu
AU - Chowdhuri, Malay Bikas
AU - Dong, Chunfeng
AU - Zhou, Hangyu
AU - Cui Zhengying, Zhengying
AU - Fujii, Keisuke
AU - Furuzawa, Akihiro
AU - Hasuo, Masahiro
AU - Iwamae, Atsushi
AU - Jie, Yinxian
AU - Koubiti, Mohammed
AU - Sakurai, Ikuya
AU - Tawara, Yuzuru
AU - Wan, Baonian
AU - Wu, Zhenwei
AU - Yamaguchi, Naohiro
N1 - Copyright:
Copyright 2009 Elsevier B.V., All rights reserved.
PY - 2009
Y1 - 2009
N2 - Impurity transport was investigated at both edge and core regions in large helical device (LHD) with developed spectroscopic instruments which can measure one- and two-dimensional distributions of impurities. The edge impurity behavior was studied recently using four carbon resonant transitions in different ionization stages of CIII (977Å), CIV (1548Å), CV (40.3Å) and CVI (33.7Å). When the line-averaged electron density, ne, is increased from 1 to 6 × 1013 cm-3, the ratio of (CIII+CIV)/ne increases while the ratio of (CV+CVI)/ne decreases. Here, CIII+CIV (CV+CVI) expresses the sum of CIII (CV) and CIV (CVI) intensities. The CIII+CIV indicates the carbon influx and the CV+CVI indicates the emissions through the transport in the ergodic layer. The result thus gives experimental evidence on the impurity screening by the ergodic layer in LHD, which is also supported by a three-dimensional edge particle simulation. The core impurity behavior is also studied in high-density discharges (ne ≤ 1× 1015 cm-3) with multi H2-pellets injection. It is found that the ratio of V/D (V: convection velocity, D: diffusion coefficient) decreases after pellet injection and Zeff profile shows a flat one at values of 1.1∼1.2. These results confirm no impurity accumulation occurs in high-density discharges. As a result, the iron density, nFe, is analyzed to be 6 × 10-7 ( n Fe/ne) of which the amount can be negligible as radiation source even in such high-density discharges. One- and two-dimensional impurity distributions from space-resolved VUV and EUV spectrometers newly developed for further impurity transport study are also presented with their preliminary results.
AB - Impurity transport was investigated at both edge and core regions in large helical device (LHD) with developed spectroscopic instruments which can measure one- and two-dimensional distributions of impurities. The edge impurity behavior was studied recently using four carbon resonant transitions in different ionization stages of CIII (977Å), CIV (1548Å), CV (40.3Å) and CVI (33.7Å). When the line-averaged electron density, ne, is increased from 1 to 6 × 1013 cm-3, the ratio of (CIII+CIV)/ne increases while the ratio of (CV+CVI)/ne decreases. Here, CIII+CIV (CV+CVI) expresses the sum of CIII (CV) and CIV (CVI) intensities. The CIII+CIV indicates the carbon influx and the CV+CVI indicates the emissions through the transport in the ergodic layer. The result thus gives experimental evidence on the impurity screening by the ergodic layer in LHD, which is also supported by a three-dimensional edge particle simulation. The core impurity behavior is also studied in high-density discharges (ne ≤ 1× 1015 cm-3) with multi H2-pellets injection. It is found that the ratio of V/D (V: convection velocity, D: diffusion coefficient) decreases after pellet injection and Zeff profile shows a flat one at values of 1.1∼1.2. These results confirm no impurity accumulation occurs in high-density discharges. As a result, the iron density, nFe, is analyzed to be 6 × 10-7 ( n Fe/ne) of which the amount can be negligible as radiation source even in such high-density discharges. One- and two-dimensional impurity distributions from space-resolved VUV and EUV spectrometers newly developed for further impurity transport study are also presented with their preliminary results.
UR - http://www.scopus.com/inward/record.url?scp=71449085004&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=71449085004&partnerID=8YFLogxK
U2 - 10.1088/1009-0630/11/4/07
DO - 10.1088/1009-0630/11/4/07
M3 - Article
AN - SCOPUS:71449085004
SN - 1009-0630
VL - 11
SP - 402
EP - 408
JO - Plasma Science and Technology
JF - Plasma Science and Technology
IS - 4
ER -