Introduction to Solid State Physics |
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Page 82
... specimen . On substituting for K the expression given by ( 5.37 ) , we have = ( 5.39 ) - Q = C ( T1 — T2 ) ( Av / L ) ... specimen with respect to the other end ; this excess is propagated down the specimen with an effective transport ...
... specimen . On substituting for K the expression given by ( 5.37 ) , we have = ( 5.39 ) - Q = C ( T1 — T2 ) ( Av / L ) ... specimen with respect to the other end ; this excess is propagated down the specimen with an effective transport ...
Page 89
... specimen . We imagine as a mathematical fiction a small sphere cut out of the specimen around the reference point ; then E2 is the field of the polarization charges on the inside of the cavity left by the sphere , and E3 is the field of ...
... specimen . We imagine as a mathematical fiction a small sphere cut out of the specimen around the reference point ; then E2 is the field of the polarization charges on the inside of the cavity left by the sphere , and E3 is the field of ...
Page 171
... specimen . The behavior observed in single crystals is similar to that in polycrystalline specimens . Fig . 10.7 . Schematic do- main arrange- ment for zero resultant mag- netic moment in a single crystal . Weiss explained this ...
... specimen . The behavior observed in single crystals is similar to that in polycrystalline specimens . Fig . 10.7 . Schematic do- main arrange- ment for zero resultant mag- netic moment in a single crystal . Weiss explained this ...
Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
Copyright | |
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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