• Spectroscopy and Spectral Analysis
  • Vol. 41, Issue 2, 333 (2021)
Jie SHANG, Yuan HUANG, Kai YANG, Bao-wei CHEN, Chun-hua LIU, and Yi YANG
Author Affiliations
  • [in Chinese]
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    DOI: 10.3964/j.issn.1000-0593(2021)02-0333-06 Cite this Article
    Jie SHANG, Yuan HUANG, Kai YANG, Bao-wei CHEN, Chun-hua LIU, Yi YANG. Progress of Thomson Scattering Diagnostic on HL-2A Tokamak[J]. Spectroscopy and Spectral Analysis, 2021, 41(2): 333 Copy Citation Text show less
    Layout of the HL-2A Thomson scattering system
    Fig. 1. Layout of the HL-2A Thomson scattering system
    (a) is the pulsed light used for spectral calibration, its width is about 0.8 ms and repetition time is about 4.5 ms; (b) is relative spectral responsibility of a 5-channel polychromator for Te measurement of 50 eV~3 keV
    Fig. 2. (a) is the pulsed light used for spectral calibration, its width is about 0.8 ms and repetition time is about 4.5 ms; (b) is relative spectral responsibility of a 5-channel polychromator for Te measurement of 50 eV~3 keV
    V1742B digitizers are set to sample at 2.5 GS·s-1, the time window of data acquisition is 410 ns(a) is shown the raw data of a TS signal, its FWHM is about 25 ns, and Gaussian function is utilized to fit the pulse shape (red line); (b) is displayed the laser monitor
    Fig. 3. V1742B digitizers are set to sample at 2.5 GS·s-1, the time window of data acquisition is 410 ns
    (a) is shown the raw data of a TS signal, its FWHM is about 25 ns, and Gaussian function is utilized to fit the pulse shape (red line); (b) is displayed the laser monitor
    The time interval of TS signals and laser monitor is shown for poly #7CH# denotes the index of optical channels; the TS data of 5th channel is very weak and not used
    Fig. 4. The time interval of TS signals and laser monitor is shown for poly #7
    CH# denotes the index of optical channels; the TS data of 5th channel is very weak and not used
    When the scattering signal is weak, the “intrinsic” function parameters b and c of this channel can be used to fit the pulse shape of the scattering signal
    Fig. 5. When the scattering signal is weak, the “intrinsic” function parameters b and c of this channel can be used to fit the pulse shape of the scattering signal
    Measurement results of electron temperature at core plasma for shot#34269, with NBI during 800~1 300 ms
    Fig. 6. Measurement results of electron temperature at core plasma for shot#34269, with NBI during 800~1 300 ms
    Jie SHANG, Yuan HUANG, Kai YANG, Bao-wei CHEN, Chun-hua LIU, Yi YANG. Progress of Thomson Scattering Diagnostic on HL-2A Tokamak[J]. Spectroscopy and Spectral Analysis, 2021, 41(2): 333
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