Ion Implantation and Synthesis of Materials - Studium

202 Particle Interactionsa0.8853a0L=1/22/3 2/3( Z1 + Z2).(2.22)The screening lengths presented in (2.20)–(2.22) do not differ significantly fromeach other. In all cases the screening lengths scale approximately with Z 1/3 of thecolliding atoms.ReferencesBanerjea, A., Smith, J.R.: Origins of the universal binding-energy relation. Phys. Rev. B37, 6632 (1988)Mayer, J.W., Lau, S.S.: Electronic Materials Science: For Integrated Circuits in Si andGaAs. Macmillan Publishing Company, New York (1990)Rose, J.H., Smith, J.R., Ferrante, J.: Universal binding-energy curves for metals and Bimetallicinterfaces. Phys. Rev. Lett. 47, 675 (1981)Rose, J.H., Smith, J.R., Ferrante, J.: Universal features of bonding in metals. Phys. Rev. B28, 1835 (1983)Rose, J.H., Smith, J.R., Guines, F., Ferrante, J.: Universal features of the equation of stateof metals. Phys. Rev. B 29, 2963 (1984)Torrens, I.M.: Interatomic Potentials. Academic, New York (1972)Tu, K.-N., Mayer, J.W., Feldman, L.C.: Electronic Thin Film Science for Electrical Engineersand Materials Scientists. Macmillan Publishing Company, New York (1992)Wilson, W.D., Haggmark, L.G., Biersack, J.P.: Calculations of nuclear stopping, range andstraggling in the low-energy region. Phys. Rev. B 15, 2458 (1977)Ziegler, J.F., Biersack, J.P., Littmark, U.: The Stopping and Range of Ions in Solids. PergamonPress, New York (1985)Suggested ReadingBaker, E.B.: The application of the Fermi–Thomas statistical model to the calculation ofpotential distribution in positive ions. Phys. Rev. 36, 630 (1930)Eckstein, W.: Computer Simulation of Ion–Solid Interactions, chap. 4. Springer, BerlinHeidelberg New York (1991)Feldman, L.C., Mayer, J.W.: Fundamentals of Surface and Thin Film Analysis. North-Holland, New York (1986)Fermi, E.: Eine Statistische Methode zur Bestimmung einiger Eigenschaften des Atoms undihre Anwendung auf die Theorie des periodischen Systems der Elemente. Z. Phys. 48,73 (1928)