Introduction to Solid State Physics |
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Page 134
... motion of the electrons is , to the first order in H , the same as a possible motion in the absence of H except for the superposition of a common precession of angular frequency ( 8.1 ) wLeH / 2mc , or fi = 1.40 mc / oersted ...
... motion of the electrons is , to the first order in H , the same as a possible motion in the absence of H except for the superposition of a common precession of angular frequency ( 8.1 ) wLeH / 2mc , or fi = 1.40 mc / oersted ...
Page 181
... motion by means of the spin orbit coupling , and the orbital motion in turn interacts with the crystal structure by means of the electrostatic fields and overlapping wave functions associated with neighboring atoms in the lattice . The ...
... motion by means of the spin orbit coupling , and the orbital motion in turn interacts with the crystal structure by means of the electrostatic fields and overlapping wave functions associated with neighboring atoms in the lattice . The ...
Page 305
... Motion of the boundary apparently took place by a cooperative motion of the dislocations in the array , each dislocation moving an equivalent distance in its own slip plane . Opposite top and bottom intersections of the boundary with ...
... Motion of the boundary apparently took place by a cooperative motion of the dislocations in the array , each dislocation moving an equivalent distance in its own slip plane . Opposite top and bottom intersections of the boundary with ...
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