Introduction to Solid State PhysicsProblems after each chapter. |
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Page 383
... p - n junction rectifier and the point contact and junction tran- sistors . The junction devices are in many respects easiest to discuss quantitatively , but the barrier rectifier and point contact transistor are of practical and ...
... p - n junction rectifier and the point contact and junction tran- sistors . The junction devices are in many respects easiest to discuss quantitatively , but the barrier rectifier and point contact transistor are of practical and ...
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 391
... p - n junctions or transistors . We shall first give a qualitative description of the operation of a p - n junction as a rectifier before going into the quantitative details . In a crystal containing a p - n junction we expect that in ...
... p - n junctions or transistors . We shall first give a qualitative description of the operation of a p - n junction as a rectifier before going into the quantitative details . In a crystal containing a p - n junction we expect that in ...
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