Introduction to Solid State PhysicsProblems after each chapter. |
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Page 337
... alloy . Let us consider a binary alloy AB composed of equal numbers of two types of metal atoms , A and B. The alloy is said to be ordered if the A and B atoms stand in a regular periodic arrangement with respect to one another , as in ...
... alloy . Let us consider a binary alloy AB composed of equal numbers of two types of metal atoms , A and B. The alloy is said to be ordered if the A and B atoms stand in a regular periodic arrangement with respect to one another , as in ...
Page 338
... alloy are sensitive to the degree of order . A common ordered arrangement is one in which all the nearest neighbor atoms of a B atom are A atoms , and vice versa ; this results when the dominant interaction among the atoms is a strong ...
... alloy are sensitive to the degree of order . A common ordered arrangement is one in which all the nearest neighbor atoms of a B atom are A atoms , and vice versa ; this results when the dominant interaction among the atoms is a strong ...
Page 340
... alloy . ( After Nix and Shockley . ) disorder the structure . The ferromagnetic properties of alloys may be sensitive to the degree of order ; in some cases , as in Ni3Mn , the dis- ordered alloy is weakly ferromagnetic and the ordered ...
... alloy . ( After Nix and Shockley . ) disorder the structure . The ferromagnetic properties of alloys may be sensitive to the degree of order ; in some cases , as in Ni3Mn , the dis- ordered alloy is weakly ferromagnetic and the ordered ...
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