By Robert W. Cahn and Peter Haasen (Eds.)
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B31, 1909-23. M. L. INDENBOM, 1982, Modem Crystallography II: Structure of Crystals (Springer-Verlag, Berlin). VILLARS, P. and L. D. CALVERT,1991, Pearson's Handbook of Crystallographic Data for Intermetallic Phases (American Society for Metals, USA), Vols. l to 4. , 1991, Phase Diagrams of the Elements (University of California Press, Berkeley). , and T. B. MASSALSKI, 1980, Structure of Metals, 3rd edition (Pergamon Press, Oxford). R. DE, R. BOOM, W. C. M. R. MIEDEMAand A. K. NIESSEN, 1988, Cohesion in Metals (North-Holland, Amsterdam).
H~/2m) V 2 represents the kinetic energy and v(r) the potential felt by the electron which has total energy E. ~(r) is the wave function of the electron where [~p(r)12 is the probability density of finding the electron at some point r = (x, y, z). The power of the Schr6dinger equation is illustrated by solving eq. (1) for the case of a single hydrogenic atom. It is found that solutions exist only if the wave function ~p is characterized by three distinct quantum numbers n, I and m whose significance has been discussed at the beginning of the preceding chapter.