Introduction to Solid State Physics |
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Page 292
... Holes Base : Collector Electrons Fig . 14.16 . Transistor mechanism . ( After Ryder and Kircher . ) rectification properties . Only a little hole current is required before the concentration of holes near the collector becomes ...
... Holes Base : Collector Electrons Fig . 14.16 . Transistor mechanism . ( After Ryder and Kircher . ) rectification properties . Only a little hole current is required before the concentration of holes near the collector becomes ...
Page 294
... holes to remain separated in this way unless an electric field exists in the junction region of the crystal in ... hole Potential energy of a hole 294 SEMICONDUCTORS.
... holes to remain separated in this way unless an electric field exists in the junction region of the crystal in ... hole Potential energy of a hole 294 SEMICONDUCTORS.
Page 298
... holes will diffuse across the collector barrier . If now the emitter n - p barrier is biased negatively ( in the forward direction ) with respect to the base , a relatively large forward current of electrons will flow across the reduced ...
... holes will diffuse across the collector barrier . If now the emitter n - p barrier is biased negatively ( in the forward direction ) with respect to the base , a relatively large forward current of electrons will flow across the reduced ...
Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
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absorption alkali halides alkali metal alloy anisotropy antiferromagnetic approximation atoms axes axis Bardeen barium titanate boundary calculated charge coefficient conduction band cube Curie point Debye density diamagnetic dielectric constant diffraction diffusion dipole direction discussed dislocation displacement domains effect elastic electric field entropy equation equilibrium experimental F-center factor Fermi ferroelectric ferromagnetic free electron frequency given heat capacity holes impurity interaction interstitial ionic crystals ionized lattice constant lattice points London low temperatures magnetic field magnetic moment molecules motion nearest neighbor normal observed orbital p-n junctions parallel paramagnetic particles perovskite phonons Phys physical plane polarizability polarization positive potassium chloride potential Proc quantum range order region resonance result room temperature scattering Seitz semiconductor Shockley shown in Fig single crystal sodium chloride solids specimen spin superconducting susceptibility symmetry Table theory thermal tion unit volume valence values vector velocity wave functions x-ray zero