By Frederick Seitz, David Turnbull and Henry Ehrenreich (Eds.)
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Additional info for Advances in Research
S] 7, 2059 (1962). 18 L. D. Jennings, D. R. Chipman, and J. De Marco, Phys. Rev. 136, A1612 (1964). ISM. J. Cooper, Phil. Mug. [S] 8, 811 (1963). 14 R. BRILL in metals are more spread than in free atoms. The very rough picture of the electron gas in metals would suggest an effect of this kind. Using this model, one might be tempted to determine the number of electrons belonging to the core of the atom separately. As was said already, the extrapolation of f curves to s = 0 is too uncertain for this purpose.
Therefore, is essentially the density of conduction band is a band in which the density of states vanishes below some energy. Usually the density of states is a monotonic increasing function of energy in the energy range of occupied states. The multiband and multivalley semiconductor models are of particular interest and importance because they describe the conduction bands of germanium, silicon, and the 111-V compound semiconductors. A 42 ROBERT W. KEYES states at the Fermi surface. Ordinarily, w is determined by the condition that the total number of electrons in the bands (i) must be a constant.
7. Photostriction. . . . . . . ............................. 8. Doping by Electron Irradiation. . . . . . . . . . . . . . . . . . . 9. Electronic Magnetostriction in Bismuth. . . . . . . . . . . . . . . agnetostriction and Magnetoelasticity in Germanium and ........................................................ ors . . . . . . . . . . . . 11. Effect of Donors on Ordinary Elastic Constants. . . . . . . . . . . .
Advances in Research by Frederick Seitz, David Turnbull and Henry Ehrenreich (Eds.)