Introduction to Solid State Physics |
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Page 45
Charles Kittel. After deformation the particle is at ( 3 . 6 ) r ' = xf ' + yg ' + zh ' , so
that the displacement is given by ( 3 . 7 ) 0 = r ' – 5 = x ( f ' – f ) + y ( g ' - g ) + z ( h '
– h ) . If we write the displacement as ( 3 . 8 ) Q = uf + vg + wh , we have from ( 3 .
Charles Kittel. After deformation the particle is at ( 3 . 6 ) r ' = xf ' + yg ' + zh ' , so
that the displacement is given by ( 3 . 7 ) 0 = r ' – 5 = x ( f ' – f ) + y ( g ' - g ) + z ( h '
– h ) . If we write the displacement as ( 3 . 8 ) Q = uf + vg + wh , we have from ( 3 .
Page 265
73 ) , ( 13 . 49 ) o = ( ) ( e h2 / mvp ? d ? Q . ) , where p = hk is the electronic
momentum , and we have assumed one conduction electron per atom . We now
calculate the mean square value of the ionic displacement d caused by thermal
motion ...
73 ) , ( 13 . 49 ) o = ( ) ( e h2 / mvp ? d ? Q . ) , where p = hk is the electronic
momentum , and we have assumed one conduction electron per atom . We now
calculate the mean square value of the ionic displacement d caused by thermal
motion ...
Page 301
... surface bounded by the line . Displace the material on one side of this surface
by d relative to the other side ; d is a fixed vector called the Burgers vector . In
regions where d is not parallel to the surface this relative displacement will either
...
... surface bounded by the line . Displace the material on one side of this surface
by d relative to the other side ; d is a fixed vector called the Burgers vector . In
regions where d is not parallel to the surface this relative displacement will either
...
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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