Introduction to Solid State Physicsproblems after each chapter |
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Page 241
The theory of p - n junctions is discussed in Chapter 14 . We must emphasize that
the expression o = Neʻr / m has been discussed here on a purely classical
model , with no use of quantum mechanics or quantum statistics . It will be shown
...
The theory of p - n junctions is discussed in Chapter 14 . We must emphasize that
the expression o = Neʻr / m has been discussed here on a purely classical
model , with no use of quantum mechanics or quantum statistics . It will be shown
...
Page 322
The only other metals we are in a position to treat in any detail are the transition
metals , and it is convenient to defer the discussion of these until after we have
discussed the electronic structure of simple substitutional binary alloys of the uni -
...
The only other metals we are in a position to treat in any detail are the transition
metals , and it is convenient to defer the discussion of these until after we have
discussed the electronic structure of simple substitutional binary alloys of the uni -
...
Page 525
SULFIDE PHOSPHORS Zinc and cadmium sulfides are characteristic sulfide
phosphors , and we shall discuss them ... Although the work discussed is not
universally accepted , the discussion illustrates a typical line of reasoning in this
field .
SULFIDE PHOSPHORS Zinc and cadmium sulfides are characteristic sulfide
phosphors , and we shall discuss them ... Although the work discussed is not
universally accepted , the discussion illustrates a typical line of reasoning in this
field .
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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