Introduction to Solid State Physicsproblems after each chapter |
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Page 313
The zone boundaries determined by ( 12 . 1 ) are planes normal to each G at the
midpoint . The first Brillouin zone will be formed from the shortest G ' s , of which
there are twelve given by ( 12 . 7 ) . The zone is therefore the rhombic ...
The zone boundaries determined by ( 12 . 1 ) are planes normal to each G at the
midpoint . The first Brillouin zone will be formed from the shortest G ' s , of which
there are twelve given by ( 12 . 7 ) . The zone is therefore the rhombic ...
Page 315
The zone is a possible choice of the primitive cell of a bcc lattice , and so the
volume is f ( 46 / a ) 3 = 4 ( 26 / a ) . There are then 8 / a ' states in the zone per
unit volume of crystal . A fcc crystal contains 4 / a3 atoms per unit volume , and so
we ...
The zone is a possible choice of the primitive cell of a bcc lattice , and so the
volume is f ( 46 / a ) 3 = 4 ( 26 / a ) . There are then 8 / a ' states in the zone per
unit volume of crystal . A fcc crystal contains 4 / a3 atoms per unit volume , and so
we ...
Page 316
faces of the first zone . This is essentially because the reflections from the plane
of atoms midway between the planes bounding the primitive cell will just cancel
in phase the reflections from the basal plane . We are therefore led to consider
the ...
faces of the first zone . This is essentially because the reflections from the plane
of atoms midway between the planes bounding the primitive cell will just cancel
in phase the reflections from the basal plane . We are therefore led to consider
the ...
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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 neighbor 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