Introduction to Solid State PhysicsProblems after each chapter. |
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Page 257
... f ' ( E ) is an even power of E EF , we have L1 = 0. For L2 , we have , writing x ... F ' ( E ) dE = π F ( Ep ) + ( kT ) 2F ' ' ( Ex ) + 6 The number of electrons is given by setting [ using ( 10.47 ) ] ( 10.76 ) so that Ex F ( E ) = [ * 9 ...
... f ' ( E ) is an even power of E EF , we have L1 = 0. For L2 , we have , writing x ... F ' ( E ) dE = π F ( Ep ) + ( kT ) 2F ' ' ( Ex ) + 6 The number of electrons is given by setting [ using ( 10.47 ) ] ( 10.76 ) so that Ex F ( E ) = [ * 9 ...
Page 510
... 9 7 log A 5 6 hv ( ev ) Fig . 18.7 . Evidence of the existence of excitons . The photoelectric yield y for potassium iodide with F centers is similar in form near 5.6 ev to the optical absorp- tion constant A ( arbitrary units ) for ...
... 9 7 log A 5 6 hv ( ev ) Fig . 18.7 . Evidence of the existence of excitons . The photoelectric yield y for potassium iodide with F centers is similar in form near 5.6 ev to the optical absorp- tion constant A ( arbitrary units ) for ...
Page 596
... ( 9 X 1011 ) 9 X 1011 1 / ( 9 X 1011 ) 9 X 1011 esu charge / cm2 esu conductivity coulomb / meter2 9 × 109 3 X 105 X ... F ) we have , per unit volume , ( R.3 ) = dE HdM , M. W. Zemansky , Heat and thermodynamics , McGraw - Hill Book Co ...
... ( 9 X 1011 ) 9 X 1011 1 / ( 9 X 1011 ) 9 X 1011 esu charge / cm2 esu conductivity coulomb / meter2 9 × 109 3 X 105 X ... F ) we have , per unit volume , ( R.3 ) = dE HdM , M. W. Zemansky , Heat and thermodynamics , McGraw - Hill Book Co ...
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 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 resonance result room temperature rotation semiconductor Shockley shown in Fig sodium chloride solid solution space group specimen spin superconducting surface susceptibility symmetry Table theory thermal tion transistor transition unit volume vacancies valence band values vector velocity wave functions wavelength x-ray zero