Plasma Simulation for the Anode Layer Ionization Source Using in the Material Modification Process


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Ionization source based on thruster of anode layer using on the spacecraft has been investigated greatly recently. Based on the principle and structure model of the ionization source, we introduce the Particle-In-Cell Monte-Carlo-Collision (PIC-MCC) plasma simulation method into the vacuum discharge process and study on the discharge characteristics of the ionization source. The comparison results show that the discharge characteristics of anode layer ionization source such as the beam energy, beam density change with the discharge voltage, working pressure and gas type. The discharge characteristics from simulation get a good agreement with experimental results. The simulation is instructive for further research on the optimization design and characteristics research of ionization source in the material modification process.



Edited by:

Xiao Hong Zhu, Wenlong Cheng and Li Lu




J. W. Wang et al., "Plasma Simulation for the Anode Layer Ionization Source Using in the Material Modification Process", Materials Science Forum, Vol. 932, pp. 24-29, 2018

Online since:

September 2018




* - Corresponding Author

[1] Zhang Yichen. Electron gun and ion beam technology [M], Beijing: Metallurgical Industry Press, 2004, 237-265.

[2] Sun Yao, Wang Hong. Surface Modification of Glass Substrate by Linear Ion Source [J], Journal of the Chinese Ceramic Society,2015, 11: 1561-1566.

[3] V V Zhurin, H R Kaufman R S Robinson. Physics of closed drift thrusters [J], Plasma Sources Sci. Technol. 1999, 8: 1-20.


[4] Yoshinori Nakayama, Futoshi Tanaka. Experimental Visualization of Ion Thruster Neutralization Phenomena [J], IEEE Transactions on Plasma Science, 2015, 43 (1): 269-276.


[5] Woong Chae Kim, Kie Hyung Chung, Byung Ho Choi. Characteristics of Hall effect plasma accelerator for industrial application [J], Rev. Sci. Instrum. 1994, 66(4):1356-1358.


[6] Michael Keidar, Isak I. Beilis. Electron Transport Phenomena in Plasma Devices with E×B Drift [J], IEEE Transactions on Plasma Science, 2006, 34(3): 804-814.


[7] Dong-Hee Park, Ji-Hwan Kim, Yury Ermakov,et al. Linear ion source with closed drift and extended acceleration region [J], Review of Scientific Instruments, 2008, 02B312.


[8] Birdsall C K. Particle in Cell Charged Particle Simulations, Plus Monte Carlo Collisions with Neutral Atoms, PIC-MCC [J]. IEEE Trans. Plasma Sci. 1991, 19(2): 65-85.


[9] J.P. Verboncoeur, A.B. Langdon, N.T. Gladd. An Object-oriented Electromagnetic PIC code [J], Computer Physics Communications, 1995, 87:199-211.


[10] M.T. Menzel, H.K. Stokes. User's Guide for the Poisson/Superfish Group of Codes, Los Alamos Accelerator Code Group.


[11] John E. Keem, Fort Collins. High Current Density Anode Layer Ion Sources. Veeco Instruments Inc.

[12] Zhao Jie, Tang Deli, Cheng Cangming. Study on the performance of low-power cylindrical anode layer ion source [J], Nuclear Fusion and Plasma Physics, 2009, 29 (1): 92-95.

[13] S F Geng, X M Qiu, Chinmin Cheng. Three-dimensional particle-in-cell simulation of discharge characteristics in cylindrical anode layer hall plasma accelerator [J]. Physics of Plasmas, 2012, 19(4).