Introduction to Solid State PhysicsProblems after each chapter. |
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Page 277
... band will be exactly full provided that no other bands overlap it in energy . If there are no overlapping bands , the band of interest will not contribute to electrical conductivity . All states in the band being full , an applied ...
... band will be exactly full provided that no other bands overlap it in energy . If there are no overlapping bands , the band of interest will not contribute to electrical conductivity . All states in the band being full , an applied ...
Page 278
... bands . they are divalent , because bands overlap , as indicated in Fig . 11.6 . In this way a band which might be exactly filled in the absence of overlap is not entirely filled , and a band which might be vacant in the absence of ...
... bands . they are divalent , because bands overlap , as indicated in Fig . 11.6 . In this way a band which might be exactly filled in the absence of overlap is not entirely filled , and a band which might be vacant in the absence of ...
Page 332
... Band relationships in nickel over the Curie temperature . The net magnetic moment is zero , as there are equal numbers of holes in both 3d 3d ↑ bands . and equally in the two sub - bands , the exchange interaction is dominated by ...
... Band relationships in nickel over the Curie temperature . The net magnetic moment is zero , as there are equal numbers of holes in both 3d 3d ↑ bands . and equally in the two sub - bands , the exchange interaction is dominated by ...
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