Introduction to Solid State PhysicsProblems after each chapter. |
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Page 47
... s = r . ( So s ) . The vector Sos S has a simple interpretation ( Fig . 2.3 ) as the direction of the normal to a plane ... c are the primitive translation vectors , we must have for the diffraction maxima = ( 2π / X ) ( aS ) 2πh ; ( 2.4 ) ...
... s = r . ( So s ) . The vector Sos S has a simple interpretation ( Fig . 2.3 ) as the direction of the normal to a plane ... c are the primitive translation vectors , we must have for the diffraction maxima = ( 2π / X ) ( aS ) 2πh ; ( 2.4 ) ...
Page 54
... c . ( 2.17 ) ( r ; S ) · = λ ( hu ; + kv ; + lw ; ) , so that ( 2.18 ) F ( hkl ) = [ ƒ1e12x ( hu , + kr , + tw , ) , 2 and F2 ( 2.19 ) F2 = [ f ; cos 2π ( hu ; + kv ; + lw ; ) ] 2 + [ Σ f ; sin 2π ( hu ; + kr ; + lw ; ) ] 2 . When all ...
... c . ( 2.17 ) ( r ; S ) · = λ ( hu ; + kv ; + lw ; ) , so that ( 2.18 ) F ( hkl ) = [ ƒ1e12x ( hu , + kr , + tw , ) , 2 and F2 ( 2.19 ) F2 = [ f ; cos 2π ( hu ; + kv ; + lw ; ) ] 2 + [ Σ f ; sin 2π ( hu ; + kr ; + lw ; ) ] 2 . When all ...
Page 403
... C we may determine the value of the Weiss field constant : ( 15.8 ) X - 1 = C / Te = Ng2S ( S + 1 ) μB2 / 3kTe , 2 Experimentally the susceptibility well above the Curie point is given quite accurately by C / ( T0 ) , where 0 , called ...
... C we may determine the value of the Weiss field constant : ( 15.8 ) X - 1 = C / Te = Ng2S ( S + 1 ) μB2 / 3kTe , 2 Experimentally the susceptibility well above the Curie point is given quite accurately by C / ( T0 ) , where 0 , called ...
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