Development of a Gas Cluster Ion Source and Its Application for Surface Treatment
- Authors: Pelenovich V.O.1, Zeng X.M.2, Ieshkin A.E.3, Chernysh V.S.3, Tolstogouzov A.B.2,4,5, Yang B.1, Fu D.J.2
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Affiliations:
- School of Power & Mechanical Engineering, Wuhan University
- Key Laboratory of Artificial Micro- and Nano-Materials of the Ministry of Education of China and Hubei Key Laboratory of Nuclear Solid Physics, School of Physics and Technology, Wuhan University
- Moscow State University
- Ryazan State Radio Engineering University
- Centre for Physics and Technological Research (CeFITec), Dept. de Física da Faculdade de Ciências e Tecnologia, Universidade Nova de Lisboa, Campus de Caparica
- Issue: Vol 13, No 2 (2019)
- Pages: 344-350
- Section: Article
- URL: https://journals.rcsi.science/1027-4510/article/view/196296
- DOI: https://doi.org/10.1134/S1027451019020356
- ID: 196296
Cite item
Abstract
A custom-built gas cluster ion source with an energy up to 20 keV is constructed. Ar, CO2, N2, and O2 are used as the working gases. The clusters are formed by metal conical nozzles with critical diameters of 65−135 um and a cone angle of 14°. To facilitate evacuation of the chambers we use the pulse mode of nozzle feeding. This allows an increase in the gas pressure in the stagnation zone (inlet pressure) up to 15 bar. The current of the clusters with an energy of 20 keV is 20 µA; the maximal current density is 3 µA/cm2. The mass spectra of the argon clusters formed at different pressures and electron ionization energy are studied by time-of-flight spectroscopy. The inlet pressure dependence of the mean cluster size is considered as a function of the condensation parameter Г*. An argon cluster beam is used to smooth the surface of the titanium coating and pressed silicon nanopowder. The roughness of the Ti coating surface decreases from 3.7 to 0.8 nm; the removal of microparticles from the surface is also observed. In the case of the surface of Si, besides the smoothing effect the formation of 100 nm craters is observed.
About the authors
V. O. Pelenovich
School of Power & Mechanical Engineering, Wuhan University
Author for correspondence.
Email: pelenovich@mail.ru
China, Wuhan, 430072
X. M. Zeng
Key Laboratory of Artificial Micro- and Nano-Materials of the Ministry of Education of China and Hubei Key Laboratoryof Nuclear Solid Physics, School of Physics and Technology, Wuhan University
Email: pelenovich@mail.ru
China, Wuhan, 430072
A. E. Ieshkin
Moscow State University
Email: pelenovich@mail.ru
Russian Federation, Moscow, 119991
V. S. Chernysh
Moscow State University
Email: pelenovich@mail.ru
Russian Federation, Moscow, 119991
A. B. Tolstogouzov
Key Laboratory of Artificial Micro- and Nano-Materials of the Ministry of Education of China and Hubei Key Laboratoryof Nuclear Solid Physics, School of Physics and Technology, Wuhan University; Ryazan State Radio Engineering University; Centre for Physics and Technological Research (CeFITec), Dept. de Física da Faculdade de Ciências e Tecnologia,
Universidade Nova de Lisboa, Campus de Caparica
Email: pelenovich@mail.ru
China, Wuhan, 430072; Ryazan, 390005; Caparica, 2829-516
B. Yang
School of Power & Mechanical Engineering, Wuhan University
Email: pelenovich@mail.ru
China, Wuhan, 430072
D. J. Fu
Key Laboratory of Artificial Micro- and Nano-Materials of the Ministry of Education of China and Hubei Key Laboratoryof Nuclear Solid Physics, School of Physics and Technology, Wuhan University
Email: pelenovich@mail.ru
China, Wuhan, 430072
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