Introduction to Solid State Physics |
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Page 129
A region within which the spontaneous polarization is in the same direction is
called a domain . Crystals have been grown which consist entirely of a single
domain , and this indeed is expected theoretically to be the stable configuration
for a ...
A region within which the spontaneous polarization is in the same direction is
called a domain . Crystals have been grown which consist entirely of a single
domain , and this indeed is expected theoretically to be the stable configuration
for a ...
Page 173
18 ORIGIN OF DOMAINS Now we shall show that domain structure is a natural
consequence 19 of the various contributions to the energy - exchange ,
anisotropy , and magnetic - of a ferromagnetic body . The existence of domains
may be ...
18 ORIGIN OF DOMAINS Now we shall show that domain structure is a natural
consequence 19 of the various contributions to the energy - exchange ,
anisotropy , and magnetic - of a ferromagnetic body . The existence of domains
may be ...
Page 179
The fact that a sufficiently small particle , with diameter less than 10 - 4 or 10 – 5
cm , is composed of a single domain is a result of domain theory which has been
confirmed by experiment . It can be shown 21 that with such very small particles ...
The fact that a sufficiently small particle , with diameter less than 10 - 4 or 10 – 5
cm , is composed of a single domain is a result of domain theory which has been
confirmed by experiment . It can be shown 21 that with such very small particles ...
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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