Introduction to Solid State PhysicsProblems after each chapter. |
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Page 477
... VACANCIES The simplest imperfection is a missing atom or lattice vacancy , indicated in diagrams and in chemical equations as a square ( Fig . 17.1 ) . Lattice vacancies are often known as Schottky defects . There will be a certain ...
... VACANCIES The simplest imperfection is a missing atom or lattice vacancy , indicated in diagrams and in chemical equations as a square ( Fig . 17.1 ) . Lattice vacancies are often known as Schottky defects . There will be a certain ...
Page 478
... Vacancies and vacancy clusters which play a prominent role in the theory of the alkali halides . As displayed from ... vacancies of opposite sign ; divalent ion present substitutionally with associated positive - ion vacancy ; cluster of ...
... Vacancies and vacancy clusters which play a prominent role in the theory of the alkali halides . As displayed from ... vacancies of opposite sign ; divalent ion present substitutionally with associated positive - ion vacancy ; cluster of ...
Page 490
... vacancies to enter one side more easily than the other . The vacancies may also be created or absorbed at edge dislocations and grain boundaries . In the Kirkendall effect markers are placed at the interface between an alloy ( CuZn ) ...
... vacancies to enter one side more easily than the other . The vacancies may also be created or absorbed at edge dislocations and grain boundaries . In the Kirkendall effect markers are placed at the interface between an alloy ( CuZn ) ...
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