Introduction to Solid State Physics |
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Page 13
A convenient way of choosing the unit cell is to choose an origin 0 and from it
draw the various vectors nia + n2b + nzc and then bisect each vector with a plane
perpendicular to it . The region of space which can be reached from 0 without ...
A convenient way of choosing the unit cell is to choose an origin 0 and from it
draw the various vectors nia + n2b + nzc and then bisect each vector with a plane
perpendicular to it . The region of space which can be reached from 0 without ...
Page 14
The positions of points in a unit cell are specified in terms of lattice coordinates ,
in which each coordinate is a fraction of the axial length , a , b , or c , in the
direction of the coordinate , with the origin taken at the corner of a unit cell . Thus
the ...
The positions of points in a unit cell are specified in terms of lattice coordinates ,
in which each coordinate is a fraction of the axial length , a , b , or c , in the
direction of the coordinate , with the origin taken at the corner of a unit cell . Thus
the ...
Page 16
The unit cell of the hcp structure is the hexagonal primitive cell but with an extra
atom added within the prism , so that the hcp unit cell contains two atoms .
DIAMOND STRUCTURE The space lattice of diamond is fcc with two atoms 000 ;
I 1 i ...
The unit cell of the hcp structure is the hexagonal primitive cell but with an extra
atom added within the prism , so that the hcp unit cell contains two atoms .
DIAMOND STRUCTURE The space lattice of diamond is fcc with two atoms 000 ;
I 1 i ...
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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