Introduction to Solid State Physics |
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Page 23
Writing U ( r ) dr = 4wr4p ( r ) dr as the probability that an electron lies ur
Scattering plane Fig . 1 . 16 . Calculation of the atomic scattering factor f . The
normal to the scattering plane is S . between radii r and r + dr , we have ( 1 . 11 )
sin MT dr ...
Writing U ( r ) dr = 4wr4p ( r ) dr as the probability that an electron lies ur
Scattering plane Fig . 1 . 16 . Calculation of the atomic scattering factor f . The
normal to the scattering plane is S . between radii r and r + dr , we have ( 1 . 11 )
sin MT dr ...
Page 264
where B is the amplitude ; 10 we suppose that r is sufficiently far from ro so that in
the vicinity of r the scattered wave may ' be treated as a plane wave ... Only if one
or more of the ions is displaced from its regular position do we get scattering .
where B is the amplitude ; 10 we suppose that r is sufficiently far from ro so that in
the vicinity of r the scattered wave may ' be treated as a plane wave ... Only if one
or more of the ions is displaced from its regular position do we get scattering .
Page 282
73 MOBILITY IN THE PRESENCE OF IMPURITY ATOMS When relatively few
impurity atoms are present , or at high temperatures , lattice scattering will
determine the mobility . At higher impurity concentrations , electron scattering by
impurity ...
73 MOBILITY IN THE PRESENCE OF IMPURITY ATOMS When relatively few
impurity atoms are present , or at high temperatures , lattice scattering will
determine the mobility . At higher impurity concentrations , electron scattering by
impurity ...
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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