Introduction to Solid State Physicsproblems after each chapter |
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Page 249
There is considerable interest in knowing the value of the Fermi level as a
function of the electron concentration N. The number of states ... absolute zero ,
all n values must then be filled up to ( 10.41 ) ( 8/3 ) ny } = NL } , and so ( 10.42 ) (
PL ) ?
There is considerable interest in knowing the value of the Fermi level as a
function of the electron concentration N. The number of states ... absolute zero ,
all n values must then be filled up to ( 10.41 ) ( 8/3 ) ny } = NL } , and so ( 10.42 ) (
PL ) ?
Page 356
We may obtain a general impression of the impurity levels by using an average
value of the anisotropic effective ... The dielectric constant has the value 15.8 for
germanium and 11.7 for silicon ; the values apply with fair accuracy from low ...
We may obtain a general impression of the impurity levels by using an average
value of the anisotropic effective ... The dielectric constant has the value 15.8 for
germanium and 11.7 for silicon ; the values apply with fair accuracy from low ...
Page 470
15 d ?, Хо 22 Equation ( 16.44 ) has been widely used to determine d
experimentally , and consistent values of d at a given temperature are obtained
for colloidal particles of various sizes . Results for mercury are shown in Fig . 16.9
, where ...
15 d ?, Хо 22 Equation ( 16.44 ) has been widely used to determine d
experimentally , and consistent values of d at a given temperature are obtained
for colloidal particles of various sizes . Results for mercury are shown in Fig . 16.9
, where ...
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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