Introduction to Solid State Physics |
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Page 17
There are 230 possible space groups . A full discussion of space groups is not
possible in the space available here . We shall not require knowledge of the
theory of space groups in order to understand the crystal structures explicitly
discussed ...
There are 230 possible space groups . A full discussion of space groups is not
possible in the space available here . We shall not require knowledge of the
theory of space groups in order to understand the crystal structures explicitly
discussed ...
Page 33
It is not possible to write down the successive terms by a casual inspection , nor
is it possible to sum the series conveniently . It is important so to arrange the
terms in the series that the contributions from the positive and negative terms
nearly ...
It is not possible to write down the successive terms by a casual inspection , nor
is it possible to sum the series conveniently . It is important so to arrange the
terms in the series that the contributions from the positive and negative terms
nearly ...
Page 104
It is not possible to determine the position of hydrogen atoms in a crystal by using
X - rays , because of the low scattering power of hydrogen . Neutron diffraction is
a possible tool , especially if deuterium is substituted for hydrogen .
It is not possible to determine the position of hydrogen atoms in a crystal by using
X - rays , because of the low scattering power of hydrogen . Neutron diffraction is
a possible tool , especially if deuterium is substituted for hydrogen .
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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