Introduction to Solid State PhysicsProblems after each chapter. |
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Page 333
... density of states as uniform in energy . The actual density may be quite far from uniform : Fig . 12.19 gives the results of a calculation by Koster for nickel . The width of the band is about 2.8 ev . We see the d band is characterized ...
... density of states as uniform in energy . The actual density may be quite far from uniform : Fig . 12.19 gives the results of a calculation by Koster for nickel . The width of the band is about 2.8 ev . We see the d band is characterized ...
Page 448
... density is , from ( 15.32 ) , Ua = K ( α12α22 + a22a32 + az2α12 ) . Coupling between elastic strain and magnetization direction may be taken for- mally into account by adding to the total energy density a term Uc≈ B1 ( α12exx + a22eyy ...
... density is , from ( 15.32 ) , Ua = K ( α12α22 + a22a32 + az2α12 ) . Coupling between elastic strain and magnetization direction may be taken for- mally into account by adding to the total energy density a term Uc≈ B1 ( α12exx + a22eyy ...
Page 481
... density to be expected if the densities of the two salts were purely additive . The study of the ionic conductivity is the most important single tool in the investigation of the production and mobility of lattice defects . The work of ...
... density to be expected if the densities of the two salts were purely additive . The study of the ionic conductivity is the most important single tool in the investigation of the production and mobility of lattice defects . The work of ...
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