Introduction to Solid State Physics |
From inside the book
Results 1-3 of 33
Page 9
Reflection plane . If one half of the crystal is the reflection of the other half in a
plane drawn through the center of the crystal , the crystal possesses a reflection
plane as a symmetry element . Center of inversion . A crystal possesses a center
of ...
Reflection plane . If one half of the crystal is the reflection of the other half in a
plane drawn through the center of the crystal , the crystal possesses a reflection
plane as a symmetry element . Center of inversion . A crystal possesses a center
of ...
Page 69
The wavelength at maximum reflection is known as the residual ray or Reststrahl
wavelength , and the selective reflection has been employed experimentally to
obtain narrow bands of radiation in the far infrared . Positions of the absorption ...
The wavelength at maximum reflection is known as the residual ray or Reststrahl
wavelength , and the selective reflection has been employed experimentally to
obtain narrow bands of radiation in the far infrared . Positions of the absorption ...
Page 312
If h , k , l have a common factor n , the diffracted ray may be considered either as
an nth order reflection from lattice planes with their true spacing , or else as a first
order reflection from a set of planes parallel to the true lattice planes but with a ...
If h , k , l have a common factor n , the diffracted ray may be considered either as
an nth order reflection from lattice planes with their true spacing , or else as a first
order reflection from a set of planes parallel to the true lattice planes but with a ...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
Copyright | |
13 other sections not shown
Other editions - View all
Common terms and phrases
alloy applied approximation atoms axes axis band boundary calculated cell chapter charge chloride condition conductivity consider constant crystal cubic defined dependence determined dielectric diffusion direction discussed dislocations displacement distance distribution domains effect elastic electric electron energy equal equation equilibrium example excitation experimental expression factor field force frequency function given gives heat holes interaction ionic ions lattice levels London magnetic magnetic field material mean measurements mechanism metals method molecules motion negative neighbor normal observed obtained parallel particles Phys physical plane polarization positive possible potential problem properties quantum range reference reflection region relation resistivity result room temperature scattering Show shown in Fig sodium solids space specimen stress structure suppose Table temperature theory thermal tion transition unit usually vacancy values volume wave zero