Introduction to Solid State PhysicsProblems after each chapter. |
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Page 313
... zone boundaries determined by ( 12.1 ) are planes normal to each G at the midpoint . The first Brillouin zone will be formed from the shortest G's , of which there are twelve given by ( 12.7 ) . The zone is therefore the rhombic ...
... zone boundaries determined by ( 12.1 ) are planes normal to each G at the midpoint . The first Brillouin zone will be formed from the shortest G's , of which there are twelve given by ( 12.7 ) . The zone is therefore the rhombic ...
Page 316
... zone if the structure is hexagonal close - packed ; so one often encounters a composite zone called the first Jones zone made up of the side faces of ( a ) with all parts of the second zone ( b ) above and below the lines of ...
... zone if the structure is hexagonal close - packed ; so one often encounters a composite zone called the first Jones zone made up of the side faces of ( a ) with all parts of the second zone ( b ) above and below the lines of ...
Page 326
... zone surface for the fcc lattice . The observed electron concentration of the ẞ phase ( bcc ) is close to the concentration 1.48 for which the inscribed Fermi sphere makes contact with the Brillouin zone surface for the bcc lattice ...
... zone surface for the fcc lattice . The observed electron concentration of the ẞ phase ( bcc ) is close to the concentration 1.48 for which the inscribed Fermi sphere makes contact with the Brillouin zone surface for the bcc lattice ...
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 region resonance result room temperature rotation semiconductor Shockley shown in Fig sodium chloride solid solution space group specimen spin superconducting surface susceptibility symmetry Table theory tion transition unit volume vacancies valence band values vector velocity wave functions wavelength x-ray zero