Introduction to Solid State Physicsproblems after each chapter |
From inside the book
Results 1-3 of 86
Page 241
The theory of p - n junctions is discussed in Chapter 14 . We must emphasize that
the expression o = Ne'r / m has been discussed here on a purely classical model
, with no use of quantum mechanics or quantum statistics . It will be shown later ...
The theory of p - n junctions is discussed in Chapter 14 . We must emphasize that
the expression o = Ne'r / m has been discussed here on a purely classical model
, with no use of quantum mechanics or quantum statistics . It will be shown later ...
Page 515
Conduction band It is convenient to discuss models in which the holes are
entirely E2 Trap levels trapped and a ... One type acts principally as a
recombination center as discussed in Chapter 13 , helping electrons and holes to
recombine and ...
Conduction band It is convenient to discuss models in which the holes are
entirely E2 Trap levels trapped and a ... One type acts principally as a
recombination center as discussed in Chapter 13 , helping electrons and holes to
recombine and ...
Page 525
Although the work discussed is not universally accepted , the discussion
illustrates a typical line of reasoning in this field . A model ... 98 , 909 ( 1955 ) ; the
model discussed by them is a development of models treated by M. Schön , 2.
Physik ...
Although the work discussed is not universally accepted , the discussion
illustrates a typical line of reasoning in this field . A model ... 98 , 909 ( 1955 ) ; the
model discussed by them is a development of models treated by M. Schön , 2.
Physik ...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
Copyright | |
17 other sections not shown
Other editions - View all
Common terms and phrases
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 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