Plasma and Fusion Research
Volume 19, 1402017 (2024)
Regular Articles
- Graduate School of Energy Science, Kyoto University, Uji 611-0011, Japan
- 1)
- Institute of Advanced Energy, Kyoto University, Uji 611-0011, Japan
- 2)
- National Institute for Fusion Science, Toki 509-5292, Japan
- 3)
- Graduate School of Engineering, Kyoto University, Kyoto 615-8530, Japan
Abstract
We simultaneously measured the electron temperature (Te) and electron density (ne) using a low-dispersion near-infrared spectrometer in a small-size pellet ablation cloud in Heliotron J, a medium-sized helical-axis heliotron device. We applied the intensity ratio of the Paschen-α, β, and γ to determine Te based on the collisional-radiative model, which was fairly consistent with the partial local thermodynamic equilibrium (LTE) in the upper principal quantum numbers of 4, 5, and 6. For a typical pellet injection discharge, Te and ne were determined to be 0.9 eV and 4 × 1021 m−3, respectively. Our derived generalized empirical calibration curve demonstrates a weak influence of Te on ne evaluation, particularly in the range of 0.4 - 2.0 eV. Subsequently, we determined the region where the LTE is achieved for the Paschen series.
Keywords
pellet ablation cloud, near-infrared spectroscopy, collisional-radiative model, partial LTE, electron temperature measurement, Heliotron J
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References
- [1] P.B. Parks and R.J. Turnbull, Phys. Fluids 21, 1735 (1978).
- [2] W. Houlberg et al., Nucl. Fusion 28, 595 (1988).
- [3] M. Goto et al., Plasma Phys. Control. Fusion 49, 1163 (2007).
- [4] G. Motojima et al., Rev. Sci. Instrum. 83, 093506 (2012).
- [5] G. Motojima et al., Plasma Phys. Control. Fusion 61, 075014 (2019).
- [6] A. Iwata et al., Rev. Sci. Instrum. 93, 113537 (2022).
- [7] S. Kado et al., Rev. Sci. Instrum. 89, 10D129 (2018).
- [8] K. Sawada and T. Fujimoto, J. Appl. Phys. 78, 2913 (1995).
- [9] T. Fujimoto et al., J. Appl. Phys. 66, 2315 (1989).
- [10] T. Fujimoto, Plasma Spectroscopy (Oxford University Press, USA, 2004).