Introduction to Solid State Physics |
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Page 99
19 ) P = 2wo % a3 \ m ' which gives directly the Born equation 2me ? / 1 ( 6 . 20 )
wo ? a ? Im This exhibits the connection of Ae with the residual ray frequency wo
. Values of Ae calculated by using this equation are in fairly good agreement ...
19 ) P = 2wo % a3 \ m ' which gives directly the Born equation 2me ? / 1 ( 6 . 20 )
wo ? a ? Im This exhibits the connection of Ae with the residual ray frequency wo
. Values of Ae calculated by using this equation are in fairly good agreement ...
Page 155
MACROSCOPIC EQUATIONS It is sometimes useful to consider the resonance
process in terms of the magnetic ... M for the magnetization ( magnetic moment /
volume ) and J for the angular momentum density , the classical equation of ...
MACROSCOPIC EQUATIONS It is sometimes useful to consider the resonance
process in terms of the magnetic ... M for the magnetization ( magnetic moment /
volume ) and J for the angular momentum density , the classical equation of ...
Page 213
F . and H . London 16 therefore suggested that the acceleration equation be
abandoned , and that we should take instead as the fundamental equation ( 11 .
22 ) c curl Aj = - H , which is postulated to replace Ohm ' s law in superconductors
.
F . and H . London 16 therefore suggested that the acceleration equation be
abandoned , and that we should take instead as the fundamental equation ( 11 .
22 ) c curl Aj = - H , which is postulated to replace Ohm ' s law in superconductors
.
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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