Introduction to Solid State PhysicsProblems after each chapter. |
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Page 44
... wavelength comparable with the inter- atomic spacing in crystals ; that is , we require a wavelength of the order of 1 A ( = 10-8 cm ) . Radiation of longer wavelength generally cannot resolve the details of structure on an atomic scale ...
... wavelength comparable with the inter- atomic spacing in crystals ; that is , we require a wavelength of the order of 1 A ( = 10-8 cm ) . Radiation of longer wavelength generally cannot resolve the details of structure on an atomic scale ...
Page 113
... wavelength for which the absorption is a maximum . The wavelength at maximum reflection is known as the residual ray or Reststrahl wavelength , and the selective reflection has been employed experimentally to obtain narrow bands of ...
... wavelength for which the absorption is a maximum . The wavelength at maximum reflection is known as the residual ray or Reststrahl wavelength , and the selective reflection has been employed experimentally to obtain narrow bands of ...
Page 125
... wavelength motions may have quite low frequen- cies . The long wavelength motions are particularly important at low temperatures , as there will always be modes of vibration in an infinite crystal for which he < kT , even though we may ...
... wavelength motions may have quite low frequen- cies . The long wavelength motions are particularly important at low temperatures , as there will always be modes of vibration in an infinite crystal for which he < kT , even though we may ...
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