Introduction to Solid State Physics |
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Page 175
... boundary layer . Later we shall calculate this energy and we shall find that it is of the order of 1 erg / cm2 . If ... boundary is continuous across the boundary , and no poles are formed anywhere in the crystal . As there are no poles ...
... boundary layer . Later we shall calculate this energy and we shall find that it is of the order of 1 erg / cm2 . If ... boundary is continuous across the boundary , and no poles are formed anywhere in the crystal . As there are no poles ...
Page 178
... boundary . may vary with the position of a domain boundary because of local variations in internal strains , impurities , crystallite dimensions , etc .; the variation is indicated schematically in Fig . 10.14 . In the absence of an ...
... boundary . may vary with the position of a domain boundary because of local variations in internal strains , impurities , crystallite dimensions , etc .; the variation is indicated schematically in Fig . 10.14 . In the absence of an ...
Page 179
... boundary is energetically unfavorable , frequently because too large a proportion of the volume of a small particle would be contained within the wall , the wall thick- ness being independent of the particle size . If a small particle ...
... boundary is energetically unfavorable , frequently because too large a proportion of the volume of a small particle would be contained within the wall , the wall thick- ness being independent of the particle size . If a small particle ...
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