Introduction to Solid State Physics |
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Page 13
... determined by giving the coordinates of three atoms lying in the plane . If each of the atoms lies on a crystal axis , the plane may be specified by giving the positions of the atoms along the axes in terms of the lattice constants . If ...
... determined by giving the coordinates of three atoms lying in the plane . If each of the atoms lies on a crystal axis , the plane may be specified by giving the positions of the atoms along the axes in terms of the lattice constants . If ...
Page 74
... determined by the condition that the number of states considered should come out equal to N L / a . Now km π / a as before , so that wm vokmπvo / a . = = = πυο / α . In Fig . 5.1 we compare the results given by Blackman1 for the heat ...
... determined by the condition that the number of states considered should come out equal to N L / a . Now km π / a as before , so that wm vokmπvo / a . = = = πυο / α . In Fig . 5.1 we compare the results given by Blackman1 for the heat ...
Page 179
... determined by the irregularities of the curve of boundary energy vs. displacement , and thus is determined by 21 C. Kittel , Phys . Rev. 70 , 965 ( 1946 ) ; E. C. Stoner and E. P. Wohlfarth , Trans . Roy . Soc . ( London ) A240 , 599 ...
... determined by the irregularities of the curve of boundary energy vs. displacement , and thus is determined by 21 C. Kittel , Phys . Rev. 70 , 965 ( 1946 ) ; E. C. Stoner and E. P. Wohlfarth , Trans . Roy . Soc . ( London ) A240 , 599 ...
Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
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absorption alkali alloy anisotropy antiferromagnetic approximately atoms axes axis Bardeen barium titanate boundary calculated charge coefficient conduction band cube Curie point Debye density diamagnetic dielectric constant diffraction diffusion dipole direction discussed dislocation displacement domains effect elastic electric field energy entropy equation equilibrium experimental F-centers factor Fermi ferroelectric ferromagnetic free electron frequency given heat capacity holes impurity interaction ionic crystals ionized ions lattice constant lattice points London low temperatures magnetic field magnetic moment metals molecules motion nearest neighbor normal observed optical orbital parallel paramagnetic particles perovskite phonons Phys physical plane polarizability polarization positive potassium potassium chloride potential Proc quantum resonance result room temperature scattering Seitz shear Shockley shown in Fig single crystal sodium chloride solids specimen spin strain stress superconducting surface susceptibility symmetry Table theory thermal tion transition unit volume vacancy valence values vector velocity wave functions x-ray zero