Introduction to Solid State PhysicsProblems after each chapter. |
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Page 389
... JUNCTION RECTIFICATION It is possible to produce in several ways a germanium or silicon crystal in which there are both p - type and n - type regions , with a very thin interface between them . The ... p - n JUNCTION RECTIFICATION 389.
... JUNCTION RECTIFICATION It is possible to produce in several ways a germanium or silicon crystal in which there are both p - type and n - type regions , with a very thin interface between them . The ... p - n JUNCTION RECTIFICATION 389.
Page 399
... p - n junctions , high voltage amplification will result . Power gains are as high as 50 db . The detailed theory of ... junction is nearly a perfect rectifier at room temperature , a junction transistor is nearly a perfect electronic ...
... p - n junctions , high voltage amplification will result . Power gains are as high as 50 db . The detailed theory of ... junction is nearly a perfect rectifier at room temperature , a junction transistor is nearly a perfect electronic ...
Page 400
... p - n junctions permit junction transistors to operate at very low voltage . In fact , a voltage of one or two tenths . of a volt across the collector junction will bring the collector current into the saturation range so that the ...
... p - n junctions permit junction transistors to operate at very low voltage . In fact , a voltage of one or two tenths . of a volt across the collector junction will bring the collector current into the saturation range so that the ...
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