Introduction to Solid State Physicsproblems after each chapter |
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Page 369
Charles Kittel. according to the definition of the diffusivity . Let us consider the
steady - state flow of holes from a region in which they are generated to a region
where they recombine at the rate p / tp , according to ( 13 . 44 ) . In the steady
state ...
Charles Kittel. according to the definition of the diffusivity . Let us consider the
steady - state flow of holes from a region in which they are generated to a region
where they recombine at the rate p / tp , according to ( 13 . 44 ) . In the steady
state ...
Page 393
is applied to the p region and positive to the n region , so that the potential
difference between the two regions is increased . Now practically no holes can
climb the potential hill , and the recombination current I , drops to a very small
value ; I ...
is applied to the p region and positive to the n region , so that the potential
difference between the two regions is increased . Now practically no holes can
climb the potential hill , and the recombination current I , drops to a very small
value ; I ...
Page 398
14 . 13 . JUNCTION TRANSISTORS Shockley , Sparks , and Teals have
described an important type of transistor in which transistor action takes place
within the germanium at the junctions between regions of n - type and p - type
conductivity .
14 . 13 . JUNCTION TRANSISTORS Shockley , Sparks , and Teals have
described an important type of transistor in which transistor action takes place
within the germanium at the junctions between regions of n - type and p - type
conductivity .
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Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
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alloys applied approximately associated atoms axis band boundary calculated cell chapter charge concentration condition conductivity consider constant crystal cubic density dependence determined dielectric diffusion direction discussion dislocation distribution domain effect elastic electric electron elements energy equal equation equilibrium experimental expression factor field force frequency function germanium give given heat capacity hexagonal holes important impurity increase interaction ionic ions lattice levels London magnetic magnetic field mass material measurements metals method motion neighbor normal observed obtained parallel particles Phys physics plane polarization positive possible potential problem properties range reference reflection region relation resistivity result room temperature rotation shown in Fig simple solid solution space space group specimen structure surface symmetry Table temperature theory thermal tion transition unit usually values vector volume wave zero zone