• Acta Physica Sinica
  • Vol. 69, Issue 11, 115201-1 (2020)
Wen-Qiu Li1、2、3、*, Bin Zhao1, Gang Wang1、3, and Dong Xiang4
Author Affiliations
  • 1Aerospace Information Research Institute, Chinese Academy of Sciences, Beijing 100094, China
  • 2Princeton Plasma Physics Laboratory, Princeton University, New Jersey 08543, USA
  • 3School of Electronic, Electrical and Communication Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
  • 4Beijing Institute of Aerospace Micro-electromechanical Technology, Beijing 100094, China
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    DOI: 10.7498/aps.69.20200062 Cite this Article
    Wen-Qiu Li, Bin Zhao, Gang Wang, Dong Xiang. Parametric analysis of mode coupling and liner energy deposition properties of helicon and Trivelpiece-Gould waves in helicon plasma[J]. Acta Physica Sinica, 2020, 69(11): 115201-1 Copy Citation Text show less
    Cross section of plasma column surround by conducting boundary
    Fig. 1. Cross section of plasma column surround by conducting boundary
    Influence of particle temperature on dispersion relation between helicon and TG waves: (a) Electron temperature effect; (b) ion temperature effect.
    Fig. 2. Influence of particle temperature on dispersion relation between helicon and TG waves: (a) Electron temperature effect; (b) ion temperature effect.
    The perpendicular wave number of helicon and TG waves given as functions of axial static magnetic field.
    Fig. 3. The perpendicular wave number of helicon and TG waves given as functions of axial static magnetic field.
    The perpendicular wave number of helicon and TG waves given as functions of plasma density.
    Fig. 4. The perpendicular wave number of helicon and TG waves given as functions of plasma density.
    The axial wave number of the right hand polarized wave is given as a function of (a) axial static magnetic field and (b) plasma density.
    Fig. 5. The axial wave number of the right hand polarized wave is given as a function of (a) axial static magnetic field and (b) plasma density.
    Radial power deposition profiles of the helicon and TG waves for: (a) m = 0 mode; (b) m = 1 mode.
    Fig. 6. Radial power deposition profiles of the helicon and TG waves for: (a) m = 0 mode; (b) m = 1 mode.
    Power deposition profiles of helicon and TG waves are given as functions of electron temperature for: (a) m = 0 mode; (b) m = 1 mode.
    Fig. 7. Power deposition profiles of helicon and TG waves are given as functions of electron temperature for: (a) m = 0 mode; (b) m = 1 mode.
    Power deposition profiles of helicon and TG waves are given as functions of ion temperature for: (a) m = 0 mode; (b) m = 1 mode.
    Fig. 8. Power deposition profiles of helicon and TG waves are given as functions of ion temperature for: (a) m = 0 mode; (b) m = 1 mode.
    Power deposition profiles of helicon and TG waves are given as functions of axial static magnetic field for: (a) m = 0 mode; (b) m = 1 mode.
    Fig. 9. Power deposition profiles of helicon and TG waves are given as functions of axial static magnetic field for: (a) m = 0 mode; (b) m = 1 mode.
    Power deposition profiles of helicon and TG waves are given as functions of plasma density for: (a) m = 0 mode; (b) m = 1 mode.
    Fig. 10. Power deposition profiles of helicon and TG waves are given as functions of plasma density for: (a) m = 0 mode; (b) m = 1 mode.
    Wen-Qiu Li, Bin Zhao, Gang Wang, Dong Xiang. Parametric analysis of mode coupling and liner energy deposition properties of helicon and Trivelpiece-Gould waves in helicon plasma[J]. Acta Physica Sinica, 2020, 69(11): 115201-1
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