• Spectroscopy and Spectral Analysis
  • Vol. 42, Issue 11, 3507 (2022)
Da-wei YE*, Fang DING1; *;, Ke-dong LI1; 2;, Xia-hua CHEN1; 2;, Yu LUO1; 2;, Qing ZHANG1; 2;, Ling-yi MENG1; 2;, and Guang-nan LUO1; 2;
Author Affiliations
  • 1. Institute of Plasma Physics, Hefei Institutes of Physical Science, Chinese Academy of Sciences, Hefei 230031, China
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    DOI: 10.3964/j.issn.1000-0593(2022)11-3507-05 Cite this Article
    Da-wei YE, Fang DING, Ke-dong LI, Xia-hua CHEN, Yu LUO, Qing ZHANG, Ling-yi MENG, Guang-nan LUO. Study on Time Delay of Impurity Line Emissions Between in the Edge and Core Plasmas in EAST Tokamak[J]. Spectroscopy and Spectral Analysis, 2022, 42(11): 3507 Copy Citation Text show less
    Geometry of viewing chords for the relevant diagnostics on EASTDiv-W (magenta): divertor visible spectroscopy system viewing the upper outer(UO)tungsten divertor target; EUV (black): extreme ultraviolet spectrometer viewing the core plasma; UO-LP (blue): divertor Langmuir probes at the UO target; UO-GP (green): gas puff inlet at the UO target. A typical separatrix of the main plasma is also shown with the blue line
    Fig. 1. Geometry of viewing chords for the relevant diagnostics on EAST
    Div-W (magenta): divertor visible spectroscopy system viewing the upper outer(UO)tungsten divertor target; EUV (black): extreme ultraviolet spectrometer viewing the core plasma; UO-LP (blue): divertor Langmuir probes at the UO target; UO-GP (green): gas puff inlet at the UO target. A typical separatrix of the main plasma is also shown with the blue line
    Divertor visible spectroscopy system on EAST(a): Schematic diagram of Div-W system; (b): Light path diagram viewing the UO divetor target in EAST vacuum chamber
    Fig. 2. Divertor visible spectroscopy system on EAST
    (a): Schematic diagram of Div-W system; (b): Light path diagram viewing the UO divetor target in EAST vacuum chamber
    Typical spectra measured by divertor visible spectroscopy system
    Fig. 3. Typical spectra measured by divertor visible spectroscopy system
    (a): Temporal evolutions of Ar Ⅱ line emission from the upper divertor (black), Ar ⅩⅥ line emission from the core plasma (red) and the voltage signal of piezo valve for Ar seeding (magenta); (b): Correlation coefficient ρ as a function of shift time between the Ar ⅩⅥ and the Ar Ⅱ signal; The rising time period of the spectral lines [3~4.5 s indicated by the shaded area in Fig.4 (a)] is used to calculate the correlation coefficient
    Fig. 4. (a): Temporal evolutions of Ar Ⅱ line emission from the upper divertor (black), Ar ⅩⅥ line emission from the core plasma (red) and the voltage signal of piezo valve for Ar seeding (magenta); (b): Correlation coefficient ρ as a function of shift time between the Ar ⅩⅥ and the Ar Ⅱ signal; The rising time period of the spectral lines [3~4.5 s indicated by the shaded area in Fig.4 (a)] is used to calculate the correlation coefficient
    Time traces of main plasma parameters of discharge #85263 and #85272(a): Plasma current IP; (b): Power of 4.6 GHz LHW (c): Ar Ⅱ line emission detected by Div-W, Ar ⅩⅥ line emission detected by EUV and the voltage signal of piezo valve for Ar seeding in shot #85263; (d): Ar Ⅱ emission detected by Div-W, Ar ⅩⅥ emission detected by EUV and the voltage signal of piezo valve for Ar seeding in shot #85272; (e): Electron temperature (Tet) near the outer strike point of the upper divertor
    Fig. 5. Time traces of main plasma parameters of discharge #85263 and #85272
    (a): Plasma current IP; (b): Power of 4.6 GHz LHW (c): Ar Ⅱ line emission detected by Div-W, Ar ⅩⅥ line emission detected by EUV and the voltage signal of piezo valve for Ar seeding in shot #85263; (d): Ar Ⅱ emission detected by Div-W, Ar ⅩⅥ emission detected by EUV and the voltage signal of piezo valve for Ar seeding in shot #85272; (e): Electron temperature (Tet) near the outer strike point of the upper divertor
    (a): The correlation coefficient ρ between the Ar Ⅱ signal and the Ar ⅩⅥ signal as a function of shift time of two typical discharges (#85263 and #85272) with different 4.6 GHz LHW powers; (b): Scatter graph between the maximum correlation coefficient ρ and the corresponding delay time in the similar discharges except for with different 4.6 GHz LHW powers, red for P4.6 GHz=1.5 MW and blue for P4.6 GHz=2.5 MW
    Fig. 6. (a): The correlation coefficient ρ between the Ar Ⅱ signal and the Ar ⅩⅥ signal as a function of shift time of two typical discharges (#85263 and #85272) with different 4.6 GHz LHW powers; (b): Scatter graph between the maximum correlation coefficient ρ and the corresponding delay time in the similar discharges except for with different 4.6 GHz LHW powers, red for P4.6 GHz=1.5 MW and blue for P4.6 GHz=2.5 MW
    Da-wei YE, Fang DING, Ke-dong LI, Xia-hua CHEN, Yu LUO, Qing ZHANG, Ling-yi MENG, Guang-nan LUO. Study on Time Delay of Impurity Line Emissions Between in the Edge and Core Plasmas in EAST Tokamak[J]. Spectroscopy and Spectral Analysis, 2022, 42(11): 3507
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