Introduction to Solid State Physics |
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Page 177
... materials which is subject to our control , and it is one of the most important criteria in the selection of ferromagnetic materials for practical application . The essential difference between material for permanent magnets and material ...
... materials which is subject to our control , and it is one of the most important criteria in the selection of ferromagnetic materials for practical application . The essential difference between material for permanent magnets and material ...
Page 219
... material at the boundary between nor- mal and superconducting regions will naturally be in the field Hc , but now the material outside the boundary , such as the material on the surface of the sphere , will see a field less than H , and ...
... material at the boundary between nor- mal and superconducting regions will naturally be in the field Hc , but now the material outside the boundary , such as the material on the surface of the sphere , will see a field less than H , and ...
Page 301
... material is either added to fill the gap or is subtracted to prevent overlap . Then rejoin the material on both sides , leaving the strain displacement intact at the time of the rewelding , but after- wards allowing the medium to come ...
... material is either added to fill the gap or is subtracted to prevent overlap . Then rejoin the material on both sides , leaving the strain displacement intact at the time of the rewelding , but after- wards allowing the medium to come ...
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