Introduction to Solid State Physics |
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Page 13
The region of space which can be reached from 0 without crossing any of the
planes then satisfies the requirements for a unit ... MILLER INDICES The position
and orientation of a crystal plane is determined by giving the coordinates of three
...
The region of space which can be reached from 0 without crossing any of the
planes then satisfies the requirements for a unit ... MILLER INDICES The position
and orientation of a crystal plane is determined by giving the coordinates of three
...
Page 20
matical construction and may be spoken of as the reflecting plane . If 20 is the
angle s makes with so , then 0 is the angle of incidence , and from the figure we
see that S = 2 sin 0 , as s and so are unit vectors . The phase difference ® is 27 /
1 ...
matical construction and may be spoken of as the reflecting plane . If 20 is the
angle s makes with so , then 0 is the angle of incidence , and from the figure we
see that S = 2 sin 0 , as s and so are unit vectors . The phase difference ® is 27 /
1 ...
Page 21
elementary plane geometry the direction cosines of the normal to ( hkl ) are
proportional to h / a , k / b , 1 / C . Therefore the lattice planes ( hkl ) must be
parallel to the reflecting plane , and the diffraction maxima occur when the
scattering ...
elementary plane geometry the direction cosines of the normal to ( hkl ) are
proportional to h / a , k / b , 1 / C . Therefore the lattice planes ( hkl ) must be
parallel to the reflecting plane , and the diffraction maxima occur when the
scattering ...
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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