Advanced Search+
Mohsen AFSHARMANESH, Morteza HABIBI. Directional power absorption in helicon plasma sources excited by a half-helix antenna[J]. Plasma Science and Technology, 2017, 19(10): 105403. DOI: 10.1088/2058-6272/aa8030
Citation: Mohsen AFSHARMANESH, Morteza HABIBI. Directional power absorption in helicon plasma sources excited by a half-helix antenna[J]. Plasma Science and Technology, 2017, 19(10): 105403. DOI: 10.1088/2058-6272/aa8030

Directional power absorption in helicon plasma sources excited by a half-helix antenna

More Information
  • Received Date: March 24, 2017
  • This paper deals with the investigation of the power absorption in helicon plasma excited through a half-helix antenna driven at 13.56 MHz. The simulations were carried out by means of a code, HELIC. They were carried out by taking into account different inhomogeneous radial density profiles and for a wide range of plasma densities, from 1011 cm-3 to 1013 cm-3. The magnetic field was 200, 400, 600 and 1000 G. A three-parameter function was used for generating various density profiles with different volume gradients, edge gradients and density widths. The density profile had a large effect on the efficient Trivelpiece–Gould (TG) and helicon mode excitation and antenna coupling to the plasma. The fraction of power deposition via the TG mode was extremely dependent on the plasma density near the plasma boundary. Interestingly, the obtained efficient parallel helicon wavelength was close to the anticipated value for Gaussian radial density profile. Power deposition was considerably asymmetric when the n/B0ratio was more than a specific value for a determined density width. The longitudinal power absorption was symmetric at approximately n0 =1011cm-3, irrespective of the magnetic field supposed. The asymmetry became more pronounced when the plasma density was 10 12cm-3. The ratio of density width to the magnetic field was an important parameter in the power coupling. At high magnetic fields, the maximum of the power absorption was reached at higher plasma density widths. There was at least one combination of the plasma density, magnetic field and density width for which the RF power deposition at both side of the tube reached its maximum value.
  • [1]
    Brog G G and Boswell R W 1998 Phys. Plasmas 5 564
    [2]
    Kr?mer M, Lorenz B and Clarenbach B 2002 Plasma Sources Sci. Technol. 11 A120
    [3]
    Chi K K, Sheridan T E and Boswell R W 1999 Plasma Sources Sci. Technol. 8 421
    [4]
    Enk T and Kr?mer M 2000 Phys. Plasmas 7 4308
    [5]
    Jung H D et al 2004 Rev. Sci. Instrum. 75 1878
    [6]
    Jung H D et al 2007 IEEE Tran. Plasma Sci. 35 1476
    [7]
    Miljak D G and Chen F F 1998 Plasma Sources Sci. Technol. 7 61
    [8]
    Kr?mer M 1999 Phys. Plasmas 6 1052
    [9]
    Sherdian T E and Chi K K 2000 Phys. Lett. A271 391
    [10]
    Niemi K and Kr?mer M 2008 Phys. Plasmas 15 073503
    [11]
    Kr?mer M, Enk T and Lorenz B 2000 Phys. Scr. 2000 132
    [12]
    Cho S and Kwak J G 1997 Phys. Plasmas 4 4167
    [13]
    Aliey Y M and Kr?mer M 2016 Phys. Plasmas 23 103505
    [14]
    Gosh S et al 2015 Plasma Sources Sci. Technol. 24 034011
    [15]
    Stenzel R L and Urritia J M 2016 Phys. Plasmas 23 092103
    [16]
    Isayama S et al 2016 Phys. Plasmas 23 063513
    [17]
    Chen F F and Arnush D 1997 Phys. Plasmas 4 3411
    [18]
    Chen F F and Arnush D 1998 Phys. Plasmas 5 1239
    [19]
    Arnush D 2000 Phys. Plasmas 7 3042
    [20]
    Mouzouris Y and Scharer J E 1996 IEEE Trans. Plasma Sci. 24 152
    [21]
    Melazzi D et al 2012 Comput. Phys. Commun. 183 1182
    [22]
    Melazzi D and Lancellotti V 2015 Plasma Sources Sci. Technol. 24 025024
    [23]
    Stix T H 1962 The Theory of Plasma Waves (New York: McGraw-Hill)
    [24]
    Boswell R W 1984 Plasma Phys. Control. Fusion 26 1147
    [25]
    Reilly M P and Miley G H 2010 Plasma Sources Sci. Technol. 19 045006
    [26]
    Eom G S and Choe W 2002 J. Vac. Sci. Technol. 20 2079
    [27]
    Chabert P and Braithwaite N 2011 Physics of Radio-Frequency Plasmas (New York: Cambridge University Press)
  • Related Articles

    [1]Kunihiro OGAWA, Mitsutaka ISOBE, Takeo NISHITANI, Sadayoshi MURAKAMI, Ryosuke SEKI, Hideo NUGA, Neng PU, Masaki OSAKABE, LHD Experiment Group. Study of first orbit losses of 1 MeV tritons using the Lorentz orbit code in the LHD[J]. Plasma Science and Technology, 2019, 21(2): 25102-025102. DOI: 10.1088/2058-6272/aaeba8
    [2]Linghan WAN (万凌寒), Zhoujun YANG (杨州军), Ruobing ZHOU (周若冰), Xiaoming PAN (潘晓明), Chi ZHANG (张弛), Xianli XIE (谢先立), Bowen RUAN (阮博文). Design of Q-band FMCW reflectometry for electron density profile measurement on the Joint TEXT tokamak[J]. Plasma Science and Technology, 2017, 19(2): 25602-025602. DOI: 10.1088/2058-6272/19/2/025602
    [3]JIANG Peng (江澎), LIN Zhihong (林志宏), Ihor HOLOD, XIAO Chijie (肖池阶). The Implementation of Magnetic Islands in Gyrokinetic Toroidal Code[J]. Plasma Science and Technology, 2016, 18(2): 126-130. DOI: 10.1088/1009-0630/18/2/05
    [4]QU Hao (屈浩), ZHANG Tao (张涛), ZHANG Shoubiao (张寿彪), WEN Fei (文斐), WANG Yumin (王嵎民), KONG Defeng (孔德峰), HAN Xiang (韩翔), YANG Yao (杨曜), GAO Yu (高宇), HUANG Canbin (黄灿斌), CAI Jianqing (蔡剑青), GAO Xiang (高翔), the EAST team. Q-Band X-Mode Reflectometry and Density Profile Reconstruction[J]. Plasma Science and Technology, 2015, 17(12): 985-990. DOI: 10.1088/1009-0630/17/12/01
    [5]HU Yixiang(呼义翔), ZENG Jiangtao(曾江涛), SUN Fengju(孙凤举), WEI Hao(魏浩), YIN Jiahui(尹佳辉), CONG Peitian(丛培天), QIU Aici(邱爱慈). Modeling Methods for the Main Switch of High Pulsed-Power Facilities Based on Transmission Line Code[J]. Plasma Science and Technology, 2014, 16(9): 873-876. DOI: 10.1088/1009-0630/16/9/12
    [6]ZHAO Qing(赵青), XING Xiaojun(邢晓俊), XUAN Yinliang(宣银良), LIU Shuzhang(刘述章). The Influence of Magnetic Field on Antenna Performance in Plasma[J]. Plasma Science and Technology, 2014, 16(6): 614-619. DOI: 10.1088/1009-0630/16/6/14
    [7]ZHANG Shoubiao(张寿彪), GAO Xiang(高翔), LING Bili(凌必利), WANG Yumin(王嵎民), ZHANG Tao(张涛), HAN Xiang(韩翔), LIU Zixi(刘子奚), BU Jingliang(布景亮), LI Jiangang(李建刚), EAST team. Density Profile and Fluctuation Measurements by Microwave Reflectometry on EAST[J]. Plasma Science and Technology, 2014, 16(4): 311-315. DOI: 10.1088/1009-0630/16/4/02
    [8]ZHANG Chongyang (张重阳), LIU Ahdi (刘阿娣), LI Hong (李弘), LI Bin (李斌), et al.. X-Mode Frequency Modulated Density Profile Reflectometer on EAST Tokamak[J]. Plasma Science and Technology, 2013, 15(9): 857-862. DOI: 10.1088/1009-0630/15/9/04
    [9]XI Yanbin (奚衍斌), LIU Yue (刘悦). FDTD Simulation on Power Absorption of Terahertz Electromagnetic Waves in Dense Plasma[J]. Plasma Science and Technology, 2012, 14(1): 5-8. DOI: 10.1088/1009-0630/14/1/02
    [10]LI Bin, LI Hong, CHEN Zhipeng, XIE Jinlin, FENG Guangyao, LIU Wandong. Experimental and Simulational Studies on the Theoretical Model of the Plasma Absorption Probe[J]. Plasma Science and Technology, 2010, 12(5): 513-518.

Catalog

    Article views (254) PDF downloads (638) Cited by()

    /

    DownLoad:  Full-Size Img  PowerPoint
    Return
    Return