Introduction to Solid State Physics |
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Page 89
Dielectric Properties In this chapter we discuss first the relationship between the
applied electric field and the local electric field acting on an atom . The interaction
of the local field with the atom determines the polarization , yet the local field ...
Dielectric Properties In this chapter we discuss first the relationship between the
applied electric field and the local electric field acting on an atom . The interaction
of the local field with the atom determines the polarization , yet the local field ...
Page 90
If we are far enough away from the individual dipoles of a uniformly polarized
specimen , we may , according to an elementary transformation occurring in
electrostatic theory , calculate the field of the specimen as equal to the field of a
surface ...
If we are far enough away from the individual dipoles of a uniformly polarized
specimen , we may , according to an elementary transformation occurring in
electrostatic theory , calculate the field of the specimen as equal to the field of a
surface ...
Page 156
We may picture the magnetization vector as precessing about the static field at an
angle which depends on the amplitude of the r - f field , on the proximity to
resonance , and on damping factors which we have not introduced here .
We may picture the magnetization vector as precessing about the static field at an
angle which depends on the amplitude of the r - f field , on the proximity to
resonance , and on damping factors which we have not introduced here .
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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