• Chinese Optics Letters
  • Vol. 13, Issue Suppl., S21202 (2015)
Yingying Li1、*, Xianghui Yin1、2, Bangxin Wang3、**, Yi Zhang1、2, Jia Fu1, and Bo Lv1
Author Affiliations
  • 1Institute of Plasma Physics, Chinese Academy of Sciences, Hefei 230031, China
  • 2School of Nuclear Science and Technology, University of Science and Technology of China, Hefei 230026, China
  • 3Key Laboratory of Atmospheric Composition and Optical Radiation, Anhui Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Hefei 230031, China
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    DOI: 10.3788/COL201513.S21202 Cite this Article Set citation alerts
    Yingying Li, Xianghui Yin, Bangxin Wang, Yi Zhang, Jia Fu, Bo Lv. Design of filter spectroscopy for the measurement of plasma ion temperature and rotation on the Experimental Advanced Superconducting Tokamak tokamak[J]. Chinese Optics Letters, 2015, 13(Suppl.): S21202 Copy Citation Text show less
    Schematic for the principle of the charge exchange recombination (left). Right, CXRS spectrum; Doppler shift (ΔλD), width (ΔλFWHM), and intensity of the spectral line give information on the rotation velocity, temperature, and density of the observed species. Remainder, reference wavelength of CVI (n=8→7) is 529.05 nm.
    Fig. 1. Schematic for the principle of the charge exchange recombination (left). Right, CXRS spectrum; Doppler shift (ΔλD), width (ΔλFWHM), and intensity of the spectral line give information on the rotation velocity, temperature, and density of the observed species. Remainder, reference wavelength of CVI (n=87) is 529.05 nm.
    Top view of the filter spectrometer optical layout. Designed center wavelength for the three filters (Channel 3) is 529.55 nm, the tilt angle of the silica filter for the two short wavelength (529.05 and 528.55 nm; Channels 2 and 1, respectively) is about 3.6° and 5.1°, respectively.
    Fig. 2. Top view of the filter spectrometer optical layout. Designed center wavelength for the three filters (Channel 3) is 529.55 nm, the tilt angle of the silica filter for the two short wavelength (529.05 and 528.55 nm; Channels 2 and 1, respectively) is about 3.6° and 5.1°, respectively.
    Schematic representation of the measurement principle of filter spectroscopy. Three Gaussian functions with different central wavelength and width are used to represent the spectral sensitivity and a slight difference for each channel is assumed.
    Fig. 3. Schematic representation of the measurement principle of filter spectroscopy. Three Gaussian functions with different central wavelength and width are used to represent the spectral sensitivity and a slight difference for each channel is assumed.
    Ion temperature and rotation velocity dependence of the line intensity ratios RL and RR as calculated with Eq. (4).
    Fig. 4. Ion temperature and rotation velocity dependence of the line intensity ratios RL and RR as calculated with Eq. (4).
    Yingying Li, Xianghui Yin, Bangxin Wang, Yi Zhang, Jia Fu, Bo Lv. Design of filter spectroscopy for the measurement of plasma ion temperature and rotation on the Experimental Advanced Superconducting Tokamak tokamak[J]. Chinese Optics Letters, 2015, 13(Suppl.): S21202
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