Introduction to Solid State Physicsproblems after each chapter |
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Page 2
We assume that a is the shortest non - vanishing translation in the translation
group . We choose coordinate axes so that a is parallel to the x axis . If now we
rotate a by an angle d , we get a new vector a ' with components az ' = a cos ; ay '
= a ...
We assume that a is the shortest non - vanishing translation in the translation
group . We choose coordinate axes so that a is parallel to the x axis . If now we
rotate a by an angle d , we get a new vector a ' with components az ' = a cos ; ay '
= a ...
Page 50
The vector r * ( hkl ) in the reciprocal lattice is in the same direction but n times as
long as the vector corresponding to the true crystal plane . That is , the nth point
from the origin in a given row in the reciprocal lattice corresponds to the nth order
...
The vector r * ( hkl ) in the reciprocal lattice is in the same direction but n times as
long as the vector corresponding to the true crystal plane . That is , the nth point
from the origin in a given row in the reciprocal lattice corresponds to the nth order
...
Page 545
The resulting strain pattern is that of the dislocation characterized jointly by the
boundary curve and the Burgers vector . It is clear that the Burgers vector must be
one of a discrete set of lattice vectors that will allow the rewelding process to ...
The resulting strain pattern is that of the dislocation characterized jointly by the
boundary curve and the Burgers vector . It is clear that the Burgers vector must be
one of a discrete set of lattice vectors that will allow the rewelding process to ...
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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