Introduction to Solid State Physicsproblems after each chapter |
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Page 200
14 FERROELECTRIC DOMAINS We have seen that a crystal of barium titanate
has cubic symmetry above the Curie point and tetragonal ... A region within which
the spontaneous polarization is in the same direction is called a domain .
14 FERROELECTRIC DOMAINS We have seen that a crystal of barium titanate
has cubic symmetry above the Curie point and tetragonal ... A region within which
the spontaneous polarization is in the same direction is called a domain .
Page 417
The existence of domains may be inferred from the character of the
magnetization curve itself . But the most direct evidence of domain structure is
furnished by photomicrographs of domain boundaries obtained by the technique
of magnetic ...
The existence of domains may be inferred from the character of the
magnetization curve itself . But the most direct evidence of domain structure is
furnished by photomicrographs of domain boundaries obtained by the technique
of magnetic ...
Page 422
case arises from magnetostriction : since the closure domains are magnetized
along different axes from the basic ... the simple cases we have discussed , but
domain structure always has its origin in the possibility of lowering the energy of
a ...
case arises from magnetostriction : since the closure domains are magnetized
along different axes from the basic ... the simple cases we have discussed , but
domain structure always has its origin in the possibility of lowering the energy of
a ...
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Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
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alloys applied approximately associated atoms axis band boundary calculated cell chapter charge concentration condition conductivity consider constant crystal cubic density dependence determined dielectric diffusion direction discussion dislocation distribution domain effect elastic electric electron elements energy equal equation equilibrium experimental expression factor field force frequency function germanium give given heat capacity hexagonal holes important impurity increase interaction ionic ions lattice levels London magnetic mass material measurements metals method motion normal observed obtained parallel particles Phys physics plane polarization positive possible potential present problem properties range reference reflection region relation resistivity result room temperature rotation shown in Fig simple solid solution space space group specimen structure surface symmetry Table temperature theory thermal tion transition unit usually values vector volume wave zero zone