Introduction to Solid State Physics |
From inside the book
Results 1-3 of 29
Page 292
Transistor action depends on the fact that the current from the emitter is
composed largely of positive holes . 10 The holes are attracted to the collector
point by the electric field in the germanium arising from the current flowing to the
collector ...
Transistor action depends on the fact that the current from the emitter is
composed largely of positive holes . 10 The holes are attracted to the collector
point by the electric field in the germanium arising from the current flowing to the
collector ...
Page 294
neutralize the space charge of the donor ions , while similarly the holes
contributed by the acceptor ions will be found chiefly in the p - region . It is not
possible for the electrons and holes to remain separated in this way unless an
electric field ...
neutralize the space charge of the donor ions , while similarly the holes
contributed by the acceptor ions will be found chiefly in the p - region . It is not
possible for the electrons and holes to remain separated in this way unless an
electric field ...
Page 298
base electrode ( “ reverse " direction for collector p - n junction ) , only a small
back current of electron and holes will diffuse across the collector barrier . If now
the emitter n - p barrier is biased negatively in the forward direction ) with respect
to ...
base electrode ( “ reverse " direction for collector p - n junction ) , only a small
back current of electron and holes will diffuse across the collector barrier . If now
the emitter n - p barrier is biased negatively in the forward direction ) with respect
to ...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
Copyright | |
13 other sections not shown
Other editions - View all
Common terms and phrases
alloy applied approximation atoms axes axis band boundary calculated cell chapter charge chloride condition conductivity consider constant crystal cubic defined dependence determined dielectric diffusion direction discussed dislocations displacement distance distribution domains effect elastic electric electron energy equal equation equilibrium example excitation experimental expression factor field force frequency function given gives heat holes interaction ionic ions lattice levels London magnetic magnetic field material mean measurements mechanism metals method molecules motion negative neighbor normal observed obtained parallel particles Phys physical plane polarization positive possible potential problem properties quantum range reference reflection region relation resistivity result room temperature scattering Show shown in Fig sodium solids space specimen stress structure suppose Table temperature theory thermal tion transition unit usually vacancy values volume wave zero