Introduction to Solid State Physicsproblems after each chapter |
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Page 310
It is important to observe LiK that the width of emission band should be a good
measure of the width of the filled portion ... The method may also be applied to
non - metals : the observed width of the filled valence band in diamond is 33 + 3
ev ...
It is important to observe LiK that the width of emission band should be a good
measure of the width of the filled portion ... The method may also be applied to
non - metals : the observed width of the filled valence band in diamond is 33 + 3
ev ...
Page 367
Shockley has calculated minority carrier lifetimes of the order of 1 sec for the
radiative process in germanium at room temperature ; overall observed lifetimes
are reported to be of the order of 0.01 sec in unusually pure germanium crystals
and ...
Shockley has calculated minority carrier lifetimes of the order of 1 sec for the
radiative process in germanium at room temperature ; overall observed lifetimes
are reported to be of the order of 0.01 sec in unusually pure germanium crystals
and ...
Page 568
Herring and Galt33 have observed in this connection that whiskers of tin ( radius
~ 10-4 cm ) have elastic Fig . 19.22 . Iron wiskers grown from the vapor by
hydrogen reduction of ferrous bromide at 710 ° C in an iron boat . ( Courtesy of S.
Herring and Galt33 have observed in this connection that whiskers of tin ( radius
~ 10-4 cm ) have elastic Fig . 19.22 . Iron wiskers grown from the vapor by
hydrogen reduction of ferrous bromide at 710 ° C in an iron boat . ( Courtesy of S.
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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