Introduction to Solid State Physics |
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Page 117
8 X 10 - 10 ) ~ 0 . 15 X 10 ^ 8 cm , which is a reasonable magnitude . We
suppose that the Curie point is determined approximately by the interaction
energy of a dipole with the local internal electric field caused by the polarization
itself .
8 X 10 - 10 ) ~ 0 . 15 X 10 ^ 8 cm , which is a reasonable magnitude . We
suppose that the Curie point is determined approximately by the interaction
energy of a dipole with the local internal electric field caused by the polarization
itself .
Page 148
When the spin orbit interaction energy is introduced as an additional perturbatior
on the system , the quenching may be partially lifted as the spin may carry some
orbital moment along with it . If the sign of the spin orbit interaction favors parallel
...
When the spin orbit interaction energy is introduced as an additional perturbatior
on the system , the quenching may be partially lifted as the spin may carry some
orbital moment along with it . If the sign of the spin orbit interaction favors parallel
...
Page 196
The exchange interactions A – A , B – B , and A – B are all antiferromagnetic , but
the A – B interaction is usually considerably the strongest , so that the A and B
lattices are individually ferromagnetic but with the magnetizations MA ...
The exchange interactions A – A , B – B , and A – B are all antiferromagnetic , but
the A – B interaction is usually considerably the strongest , so that the A and B
lattices are individually ferromagnetic but with the magnetizations MA ...
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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