Introduction to Solid State PhysicsProblems after each chapter. |
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Page 108
... solution for k = T / L has usin nra / L and vanishes for n = 0 and n = N as required , with a maximum for n = N / 2 . The solution for k = NT / LT / a = km has ua sin na , permitting no motion at all , because sin në vanishes at each ...
... solution for k = T / L has usin nra / L and vanishes for n = 0 and n = N as required , with a maximum for n = N / 2 . The solution for k = NT / LT / a = km has ua sin na , permitting no motion at all , because sin në vanishes at each ...
Page 274
... solution is eix / a ± eirra . The evolution of the standing wave solution is traced through in detail in Appendix I. What is important at present is that the solutions for k / a combine to give standing waves of different energies , the ...
... solution is eix / a ± eirra . The evolution of the standing wave solution is traced through in detail in Appendix I. What is important at present is that the solutions for k / a combine to give standing waves of different energies , the ...
Page 322
... solutions to occur . He suggests that the solid solution range is very restricted if the atomic diameters of solvent and solute differ by more than 15 percent . The atomic diameter for this purpose is usually taken as the closest ...
... solutions to occur . He suggests that the solid solution range is very restricted if the atomic diameters of solvent and solute differ by more than 15 percent . The atomic diameter for this purpose is usually taken as the closest ...
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