Introduction to Solid State Physicsproblems after each chapter |
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Page 18
Reflection planes are indicated by heavy lines . If there is present a reflection
plane normal to the principal axis , the outer circle is heavy on the symmetry
element stereogram . Symmetry axes perpendicular to the principal axis are
denoted by ...
Reflection planes are indicated by heavy lines . If there is present a reflection
plane normal to the principal axis , the outer circle is heavy on the symmetry
element stereogram . Symmetry axes perpendicular to the principal axis are
denoted by ...
Page 48
We recall that a , b , y are the direction cosines of S , the normal to the reflecting
plane , referred to the basis vectors a , b ... maxima occur when the scattering
direction may be derived from the incident direction by reflection in a lattice plane
.
We recall that a , b , y are the direction cosines of S , the normal to the reflecting
plane , referred to the basis vectors a , b ... maxima occur when the scattering
direction may be derived from the incident direction by reflection in a lattice plane
.
Page 271
We have seen in the earlier discussions of x - ray and elastic wave propagation
in crystals that Bragg reflection is an important and characteristic feature of wave
propagation in periodic structures . Bragg reflection occurs also for electron ...
We have seen in the earlier discussions of x - ray and elastic wave propagation
in crystals that Bragg reflection is an important and characteristic feature of wave
propagation in periodic structures . Bragg reflection occurs also for electron ...
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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