Introduction to Solid State PhysicsProblems after each chapter. |
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Page 351
... determined for a number of substances are given in Table 13.1 . Many of the values were determined from the slope of plots of log o vs. 1 / T ; some of the other values were determined from the long wavelength limit of the optical ...
... determined for a number of substances are given in Table 13.1 . Many of the values were determined from the slope of plots of log o vs. 1 / T ; some of the other values were determined from the long wavelength limit of the optical ...
Page 371
... determine experimen- tally the form of the energy surfaces of the conduction and valence bands near the band edges ; that is , the energy E ( k ) is determined as a function of the wave vector k . The determination of the energy sur ...
... determine experimen- tally the form of the energy surfaces of the conduction and valence bands near the band edges ; that is , the energy E ( k ) is determined as a function of the wave vector k . The determination of the energy sur ...
Page 488
... determined directly by this method with values determined from observed conductivities with the use of the Einstein relation . It is found that the two sets of values do not usually agree within the experimental accuracy , suggesting ...
... determined directly by this method with values determined from observed conductivities with the use of the Einstein relation . It is found that the two sets of values do not usually agree within the experimental accuracy , suggesting ...
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 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