Introduction to Solid State Physics |
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Page 16
DIAMOND STRUCTURE The space lattice of diamond is fcc with two atoms 000 ;
I 1 i associated with each lattice point . ... The hexagonal Taking each one of the
fourteen space close - packed structure . lattices , we can associate with every ...
DIAMOND STRUCTURE The space lattice of diamond is fcc with two atoms 000 ;
I 1 i associated with each lattice point . ... The hexagonal Taking each one of the
fourteen space close - packed structure . lattices , we can associate with every ...
Page 311
Appendix A . INTERFERENCE CONDITIONS AND THE RECIPROCAL LATTICE
The conditions for an x - ray beam to be diffracted by a crystal may be expressed
in an elegant form with the help of the reciprocal lattice transformation .
Appendix A . INTERFERENCE CONDITIONS AND THE RECIPROCAL LATTICE
The conditions for an x - ray beam to be diffracted by a crystal may be expressed
in an elegant form with the help of the reciprocal lattice transformation .
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 ...
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Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
Copyright | |
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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