Introduction to Solid State PhysicsProblems after each chapter. |
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Page 69
... alkali metal crystal is seen from Table 3.1 to be very considerably less than that of an alkali halide crystal , so the bond formed by a quasi - free conduction electron is not very strong . Part of the explanation is that the ...
... alkali metal crystal is seen from Table 3.1 to be very considerably less than that of an alkali halide crystal , so the bond formed by a quasi - free conduction electron is not very strong . Part of the explanation is that the ...
Page 317
... ALKALI METALS BAND STRUCTURE OF METALS The alkali atoms have one s valence electron on each atom : 2s in lithium , 3s in sodium , 4s in potassium , 5s in rubidium , and 6s in cesium . In the alkali metals , the s levels are spread out ...
... ALKALI METALS BAND STRUCTURE OF METALS The alkali atoms have one s valence electron on each atom : 2s in lithium , 3s in sodium , 4s in potassium , 5s in rubidium , and 6s in cesium . In the alkali metals , the s levels are spread out ...
Page 480
... alkali halides the most common lattice vacancies are Schottky defects while in pure silver halides the most common vacancies arise from Frenkel defects . We note that the production of Schottky defects lowers the density of the crystal ...
... alkali halides the most common lattice vacancies are Schottky defects while in pure silver halides the most common vacancies arise from Frenkel defects . We note that the production of Schottky defects lowers the density of the crystal ...
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