Introduction to Solid State PhysicsProblems after each chapter. |
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Page 234
Charles Kittel. 10 Free Electron Model of Metals It is possible to understand a number of important physical proper- ties of some metals , in particular the simple monovalent metals , in terms of the free electron model . According to ...
Charles Kittel. 10 Free Electron Model of Metals It is possible to understand a number of important physical proper- ties of some metals , in particular the simple monovalent metals , in terms of the free electron model . According to ...
Page 266
... free electrons , mass m ) ( A ) Effective mass ratio m * / m , according to Brooks ( see Chapter 11 ) Ao ( calculated for m * ) ( A ) A observed ( A ) Li Na K Rb Cs 1550 2090 2870 3220 3620 1.40 0.98 0.94 ... FREE ELECTRON MODEL OF METALS.
... free electrons , mass m ) ( A ) Effective mass ratio m * / m , according to Brooks ( see Chapter 11 ) Ao ( calculated for m * ) ( A ) A observed ( A ) Li Na K Rb Cs 1550 2090 2870 3220 3620 1.40 0.98 0.94 ... FREE ELECTRON MODEL OF METALS.
Page 270
... free electron model is quite uninstructive . The model cannot help us understand why some chemical elements crystallize to form good conductors of electricity and others to form insulators ; still others are semiconduc- tors , with ...
... free electron model is quite uninstructive . The model cannot help us understand why some chemical elements crystallize to form good conductors of electricity and others to form insulators ; still others are semiconduc- tors , with ...
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