2010
DOI: 10.1063/1.3326970
|View full text |Cite
|
Sign up to set email alerts
|

Z eff profile diagnostics using visible bremsstrahlung continuum for nonaxisymmetric plasmas with finite β in large helical device

Abstract: An astigmatism-corrected Czerny–Turner-type visible spectrometer coupled with a charge-coupled device has been installed in large helical device (LHD) to measure visible bremsstrahlung continuum. A full vertical profile has been observed from the elliptical plasmas at horizontally elongated plasma cross section through a 44 fiber parallel array with vertical observation length of ∼1 m. Line emissions can be easily eliminated by use of the visible spectrometer instead of an interference filter. A nonmonotonic b… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

1
11
0

Year Published

2010
2010
2021
2021

Publication Types

Select...
9

Relationship

0
9

Authors

Journals

citations
Cited by 20 publications
(12 citation statements)
references
References 21 publications
1
11
0
Order By: Relevance
“…Finally, the uncertainties of the impurity density and Z eff values in the present analysis are estimated. The errors mainly originate from the Thomson scattering measurement, the atomic model, the EUV spectrometer system, the Abel inversion process [21] , and the absolute intensity calibration [10] . The error is estimated to be 30% at most in the present study.…”
Section: Resultsmentioning
confidence: 99%
“…Finally, the uncertainties of the impurity density and Z eff values in the present analysis are estimated. The errors mainly originate from the Thomson scattering measurement, the atomic model, the EUV spectrometer system, the Abel inversion process [21] , and the absolute intensity calibration [10] . The error is estimated to be 30% at most in the present study.…”
Section: Resultsmentioning
confidence: 99%
“…One of the uncertainties is originated in the Abel inversion process. The uncertainty is estimated to be less than 5% [9]. The electron temperature measured by Thomson scattering system also brings the uncertainty, which is estimated to be less than 3%.…”
Section: Absolute Intensity Calibrationmentioning
confidence: 86%
“…The coil system consists of a set of two continuous superconducting helical coils with a poloidal pitch number of two and a toroidal pitch number of 10 and three pairs of superconducting poloidal coils. Figure 1a illustrates the top view of the shape of the plasma in the LHD device together with schematic drawings of the neutral beam injection (NBI) for heating, the impurity pellet injection, and the spectroscopic diagnostics consisting of two flat-field grazing incidence EUV spectrometers (denoted as "EUV Short" [24] and "EUV Long" [25]), a normal incidence 20 cm VUV spectrometer (denoted as "VUV 109L" [26]), and an astigmatism-corrected Czerny-Turner-type 30 cm visible spectrometer (denoted as "MK300" [27]). Neutral hydrogen atoms are used as beam particles in the experiments presented in this paper.…”
Section: Tungsten Pellet Injection Experiments In Lhdmentioning
confidence: 99%