Introduction to Solid State Physicsproblems after each chapter |
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Page 356
Further corrections for silicon have been considered by Luttinger and Kohn .
Observed values of the donor ionization energies for pentavalent impurities in
germanium and silicon are given in Table 13.3 . The values are obtained largely
by ...
Further corrections for silicon have been considered by Luttinger and Kohn .
Observed values of the donor ionization energies for pentavalent impurities in
germanium and silicon are given in Table 13.3 . The values are obtained largely
by ...
Page 362
We discuss here results obtained by Conwell and Debyes on n - type germanium
. These results will convey an impression of the kind of information which can be
obtained from a systematic analysis of conductivity and Hall data . We have ...
We discuss here results obtained by Conwell and Debyes on n - type germanium
. These results will convey an impression of the kind of information which can be
obtained from a systematic analysis of conductivity and Hall data . We have ...
Page 470
... given temperature are obtained for colloidal particles of various sizes . Results
for mercury are shown in Fig . 16.9 , where the penetration depths are compared
with those obtained by Pippard from high frequency resistance measurements .
... given temperature are obtained for colloidal particles of various sizes . Results
for mercury are shown in Fig . 16.9 , where the penetration depths are compared
with those obtained by Pippard from high frequency resistance measurements .
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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 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