Introduction to Solid State PhysicsProblems after each chapter. |
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Page 95
... equal velocities . However , the longitudinal wave velocity is not necessarily equal to the transverse wave velocity . The term in grad div gives rise to a longitudinal wave , that is , with particle displacement in the direction of the ...
... equal velocities . However , the longitudinal wave velocity is not necessarily equal to the transverse wave velocity . The term in grad div gives rise to a longitudinal wave , that is , with particle displacement in the direction of the ...
Page 180
... equal to the applied field . The correct quantum - mechanical result is larger than this by the factor 2 . 7.2 . In the local field problem the cavity need not be chosen as spherical , but may be of any shape possessing at least cubic ...
... equal to the applied field . The correct quantum - mechanical result is larger than this by the factor 2 . 7.2 . In the local field problem the cavity need not be chosen as spherical , but may be of any shape possessing at least cubic ...
Page 341
... equal to When S == ( 1 + S ) N . ± 1 , the order is perfect and each lattice contains only one type of atom . When S 0 , each lattice contains equal numbers of = A and B atoms and there is no long range order . We consider now that part ...
... equal to When S == ( 1 + S ) N . ± 1 , the order is perfect and each lattice contains only one type of atom . When S 0 , each lattice contains equal numbers of = A and B atoms and there is no long range order . We consider now that part ...
Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
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absorption acceptors alkali alloys approximately atoms axes axis barium titanate boundary Bragg Brillouin zone calculated chapter charge conduction band conduction electrons crystal structure cube cubic Curie point Debye density dielectric constant diffraction diffusion dipole direction discussion dislocation distribution domain effective mass elastic electric field energy equation equilibrium exciton experimental F centers factor Fermi ferroelectric ferromagnetic free electron frequency germanium given heat capacity hexagonal holes impurity interaction ionization ions lattice constant lattice point levels low temperatures magnetic field magnetic moment metals molecules motion nearest neighbor normal observed p-n junction paramagnetic particles phonons Phys physics plane polarizability polarization positive potential Proc region resonance result room temperature rotation semiconductor Shockley shown in Fig sodium chloride solid solution space group specimen spin superconducting surface susceptibility symmetry Table theory tion transition unit volume vacancies valence band values vector velocity wave functions wavelength x-ray zero