Introduction to Solid State PhysicsProblems after each chapter. |
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Page 370
... holes were introduced in the rod , they would drift from left to right . When the pulse generator at the left - hand point contact , or emitter point , operates , the emitter point is biased positive and causes holes to be injected into ...
... holes were introduced in the rod , they would drift from left to right . When the pulse generator at the left - hand point contact , or emitter point , operates , the emitter point is biased positive and causes holes to be injected into ...
Page 393
... holes can climb the potential hill , and the recombina- tion current I , drops to a very small value ; I , is not much affected by the reverse bias , as the distance a hole diffuses in its lifetime is large compared with the width of ...
... holes can climb the potential hill , and the recombina- tion current I , drops to a very small value ; I , is not much affected by the reverse bias , as the distance a hole diffuses in its lifetime is large compared with the width of ...
Page 513
... holes and electrons , the photon may be able to cause ionization of impurity atoms ( donor and acceptor atoms ) and in this way produce mobile electrons or holes , according to the nature of the impurity . source . Light source + Let us ...
... holes and electrons , the photon may be able to cause ionization of impurity atoms ( donor and acceptor atoms ) and in this way produce mobile electrons or holes , according to the nature of the impurity . source . Light source + Let us ...
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