Introduction to Solid State Physics |
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Page 163
TEMPERATURE DEPENDENCE OF THE SPONTANEOUS MAGNETIZATION On
the Weiss theory we must use the complete expression ( 9 . 10 ) for the
magnetization in calculating the spontaneous magnetization IM M = x . Sure - M =
NSG ...
TEMPERATURE DEPENDENCE OF THE SPONTANEOUS MAGNETIZATION On
the Weiss theory we must use the complete expression ( 9 . 10 ) for the
magnetization in calculating the spontaneous magnetization IM M = x . Sure - M =
NSG ...
Page 246
A more detailed study of the quantum theory of transport processes in metals
shows that the Lorenz number is expected to be independent of temperature only
above the Debye temperatures , 13 as the differences between the types of ...
A more detailed study of the quantum theory of transport processes in metals
shows that the Lorenz number is expected to be independent of temperature only
above the Debye temperatures , 13 as the differences between the types of ...
Page 262
In the high temperature region the calculated conductivity is proportional to T - 1 ,
and in the low temperature region it is proportional to 7 - 5 . The agreement of the
calculated temperature dependence with experiment is quite good , as shown ...
In the high temperature region the calculated conductivity is proportional to T - 1 ,
and in the low temperature region it is proportional to 7 - 5 . The agreement of the
calculated temperature dependence with experiment is quite good , as shown ...
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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