Download Advances in Research by Frederick Seitz, David Turnbull and Henry Ehrenreich (Eds.) PDF

By Frederick Seitz, David Turnbull and Henry Ehrenreich (Eds.)

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Corresponding calculations were carried out on MgO and LiF. 80 electrons for 0. These figures may be significant. 88. Because of the large V. M. Goldschmidt, Trans. 26, 253 (1929). R. Brill, C. Hermann, and C. Peters, 2. Anorg. Allgem. Chem. 261, 151 (1948). S. Togawa, J . Phys. Japan 20, 742 (1965). 33Measurements of J. Krug, H. Witte, and E. Physik. Chem. ] 4, 36 (1955). 19 ELECTRON DISTRIBUTION I N CRYSTALS dimensions of F-, an independent determination for this ion was not possible. 34The paper is concerned with the degree of ionization in LiH, where Li+ and H- are supposed to be present.

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. . .

Price, IBM Research Note NW-3 (1962) (unpublished). C. S. Smith, Phys. Rev. 94, 42 (1954). 3 Other energetically equivalent minima are generated by the symmetry operations of the crystal. The states in the vicinity of the various minima are called valleys, and the index (i) may then be used to enumerate the valleys. Scalar properties, such as the density of states function, N(O(E), are identical for all valleys. Tensor properties, such as the change in energy of a valley with some particular shear strain, are, in general, different for different vaIIeys but can be transformed from one valley to another by rotation of the coordinates.

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