Introduction to Solid State PhysicsProblems after each chapter. |
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Page 374
... ratio would have been unity . The factor one - half represents the selective absorption of one of the two circular ... ratio ( 13.65 ) σκ OR ( res ) / OR ( H = 0 ) - v2 / 2 , R provided >> 1. For wer≈ 10 , the ratio ( res ) / σR ( H v ...
... ratio would have been unity . The factor one - half represents the selective absorption of one of the two circular ... ratio ( 13.65 ) σκ OR ( res ) / OR ( H = 0 ) - v2 / 2 , R provided >> 1. For wer≈ 10 , the ratio ( res ) / σR ( H v ...
Page 409
... ratio is e / mc , so that spin ' = 2 . For orbital motion of an electron the magnetic moment z component is L2 ( eh ... ratio , but strictly speaking the gyromagnetic ratio is the reciprocal of the magnetomechanical ratio . from ( 15.16 ) ...
... ratio is e / mc , so that spin ' = 2 . For orbital motion of an electron the magnetic moment z component is L2 ( eh ... ratio , but strictly speaking the gyromagnetic ratio is the reciprocal of the magnetomechanical ratio . from ( 15.16 ) ...
Page 558
... ratio of the shear modulus to the shear stress . Since this latter ratio is of the order 103 or 104 for the yielding of most crystals , the ratio 2r / b is about the same , as assumed in making the approximation In ( r / b ) ≈ 2π ...
... ratio of the shear modulus to the shear stress . Since this latter ratio is of the order 103 or 104 for the yielding of most crystals , the ratio 2r / b is about the same , as assumed in making the approximation In ( r / b ) ≈ 2π ...
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