Introduction to Solid State Physicsproblems after each chapter |
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Page 370
If any 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 the rod .
If any 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 the rod .
Page 393
Now practically no holes can climb the potential hill , and the recombination
current I , drops to a very small value ; 1 , is not much affected by the reverse bias
, as the distance a hole diffuses in its lifetime is large compared with the width of
the ...
Now practically no holes can climb the potential hill , and the recombination
current I , drops to a very small value ; 1 , is not much affected by the reverse bias
, as the distance a hole diffuses in its lifetime is large compared with the width of
the ...
Page 513
If the energy of the incident photon is below the threshold for the production of
pairs of holes and electrons , the photon may be able to cause ionization of
impurity atoms ( donor and acceptor atoms ) and in this way produce Light source
...
If the energy of the incident photon is below the threshold for the production of
pairs of holes and electrons , the photon may be able to cause ionization of
impurity atoms ( donor and acceptor atoms ) and in this way produce Light source
...
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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 mass material measurements metals method motion normal observed obtained parallel particles Phys physics plane polarization positive possible potential present 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