Introduction to Solid State PhysicsProblems after each chapter. |
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Page 422
... materials which is subject to our control , and it is one of the most important criteria in the selection of ferromagnetic materials for practical application . The essential difference between material for permanent magnets and material ...
... materials which is subject to our control , and it is one of the most important criteria in the selection of ferromagnetic materials for practical application . The essential difference between material for permanent magnets and material ...
Page 471
... material around the equator of the sphere become normal ; the effective shape of the superconducting material will then become something like a prolate spheroid , thereby reducing the field in the interior . The material at the boundary ...
... material around the equator of the sphere become normal ; the effective shape of the superconducting material will then become something like a prolate spheroid , thereby reducing the field in the interior . The material at the boundary ...
Page 544
... material on one side of the cut is displaced relative to that on the other by vector distance b , which may be arbitrarily oriented relative to the surface . Forces will be required to effect the displacement . The medium is filled in ...
... material on one side of the cut is displaced relative to that on the other by vector distance b , which may be arbitrarily oriented relative to the surface . Forces will be required to effect the displacement . The medium is filled in ...
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