THE STUDIES OF SURFACE LAYER ATOMIC STRUCTURE OF AL(100) BY MEV ION SCATTERING

THE STUDIES OF SURFACE LAYER ATOMIC STRUCTURE OF AL(100) BY MEV ION SCATTERING

Cheng Huansheng
Cui Zhixiang
Xu Hongjie
Yao Xiaowei
Yang Fujia
Nuclear Science and TechniquesVol.1, No.1-2pp.105-112Published in print 01 May 1990
4200

A UHV system specially designed for studying surface and interface atomic structure by MeV ion scattering and channeling is described. The vacuum in the UHV chamber is 133.332×10-10Pa. The chamber is equipped with an ion gun used for sample cleaning, a translatable four-grid LEED-Auger system used for characterization of the crystal surface, and a three dimensional goniometer. The crystal preparation and cleaning procedure of Al(100) are presented. The surface peak intensity of Al(100)-< 100> and Al(100)- <100> has been measured by MeV ion channeling and scattering. The measured surface peak intensity was compared with that of Monte-Carlo simulation. The experimental results indicate that the thermal vibration amplitude of Al(100) surface atoms is 1.2-1.3 times that of bulk atoms. The relaxation of first layer for Al(100) is less than -0.005nm.

MeV ion scatteringSurface layer atomic structureAl
REFERENCES
[1] T. Narusawa et al., Phys. Rev. Lett., 47 (1981), 417.
[2] L.C. Feldman et al., Material analysis by ion channeling, Academic Press, New York, 1982.
[3] G. Mcliere, Z. Naturforsch., A2 (1947), 133.
[4] J.H. Barrett, Phys. Rev., B3 (1971), 1527.
[5] Dwight E. Gray, American institute of physics handbook, 2nd edition, 1963.
[6] R.S. Nelson et al., Phil. Mag., 7 (1962), 1385.
[7] I. Stensgard et al., Surface Sci., 77 (1978), 513.
[8] S. Rigo et al., Nucl. Instr. Meth., 149 (1978), 721.
[9] D.P. Jackson, Surface Sci., 43 (1974), 431.
[10] F. Jona et al., J. Phy. C: Solid State Phys., 13 (1980), L155.
[11] N. Masud et al., Surface Sci., 133 (1983), 580.
[12] A. Bianconi and R.Z. Bachrach, Phys. Rev. Lett., 42 (1979), 104.
[13] U. Landman et al., Phys. Rev., B21 (1980), 448.