Introduction to Solid State Physicsproblems after each chapter |
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Page 51
In the direct fcc lattice the distance between lattice planes in each cube edge
direction is a / 2 , where a is the lattice constant ; thus there are points in the
reciprocal lattice along the x , y , z axes at 2 / a from the origin . There is only one
set of ...
In the direct fcc lattice the distance between lattice planes in each cube edge
direction is a / 2 , where a is the lattice constant ; thus there are points in the
reciprocal lattice along the x , y , z axes at 2 / a from the origin . There is only one
set of ...
Page 74
6 ) " ' ; where r ; is the distance of the jth ion from the reference ion and is always
to be taken as positive . Reference ion ☺ ☺ ☺ ☺ ☺ ☺ ☺ ☺ Role Fig . 3 . 5 .
Line of ions of alternating signs with distance R , between ions . We shall first ...
6 ) " ' ; where r ; is the distance of the jth ion from the reference ion and is always
to be taken as positive . Reference ion ☺ ☺ ☺ ☺ ☺ ☺ ☺ ☺ Role Fig . 3 . 5 .
Line of ions of alternating signs with distance R , between ions . We shall first ...
Page 82
IONIC RADII It is found that the interatomic distances in the alkali halides are
approximately additive , so that to a certain extent the ions may be regarded as
rigid spheres . The distance at which the ions come into contact is the equilibrium
...
IONIC RADII It is found that the interatomic distances in the alkali halides are
approximately additive , so that to a certain extent the ions may be regarded as
rigid spheres . The distance at which the ions come into contact is the equilibrium
...
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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