Introduction to Solid State PhysicsProblems after each chapter. |
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Page 354
... impurity ; thus semiconduc- tors such as Cu2O or ZnO are known as deficit semiconductors . We consider in particular ... impurity atom in silicon ; ( a ) with arsenic impurity an electron is available for conduction ; ( b ) with boron ...
... impurity ; thus semiconduc- tors such as Cu2O or ZnO are known as deficit semiconductors . We consider in particular ... impurity atom in silicon ; ( a ) with arsenic impurity an electron is available for conduction ; ( b ) with boron ...
Page 355
... impurity atom left over after the four covalent bonds are established with the nearest neighbors , that is , after the impurity atom has been accommodated in the structure with as little disturbance as possible . The situation as shown ...
... impurity atom left over after the four covalent bonds are established with the nearest neighbors , that is , after the impurity atom has been accommodated in the structure with as little disturbance as possible . The situation as shown ...
Page 361
... IMPURITY ATOMS When relatively few impurity atoms are present , or at high tempera- tures , lattice scattering will determine the mobility . At higher impur- ity concentrations , electron scattering by impurity atoms may be important ...
... IMPURITY ATOMS When relatively few impurity atoms are present , or at high tempera- tures , lattice scattering will determine the mobility . At higher impur- ity concentrations , electron scattering by impurity atoms may be important ...
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 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