Introduction to Solid State PhysicsProblems after each chapter. |
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Page 252
... particles . As applied to electrons , quantum statistics requires that we treat all electrons as indistinguishable ... particles can have the identical energy and momentum . In the lowest state of a classical system all particles can ...
... particles . As applied to electrons , quantum statistics requires that we treat all electrons as indistinguishable ... particles can have the identical energy and momentum . In the lowest state of a classical system all particles can ...
Page 424
... Particle diameter [ microns ( 104 cm ) ] Fig . 15.17 . Coercive force of fine particles of MnBi , as a function of particle size . ( After Guillaud . ) If a small particle is constrained to remain as a single domain , it will not be ...
... Particle diameter [ microns ( 104 cm ) ] Fig . 15.17 . Coercive force of fine particles of MnBi , as a function of particle size . ( After Guillaud . ) If a small particle is constrained to remain as a single domain , it will not be ...
Page 560
... particles of Al2Cu are precipitated . If L is the mean spacing of particles on a slip plane , the stress necessary to force a dislocation between particles should be approximately ( 19.14 ) σ / G = b / L , which is ( 19.13 ) rewritten ...
... particles of Al2Cu are precipitated . If L is the mean spacing of particles on a slip plane , the stress necessary to force a dislocation between particles should be approximately ( 19.14 ) σ / G = b / L , which is ( 19.13 ) rewritten ...
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