Introduction to Solid State PhysicsProblems after each chapter. |
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Page 200
... domain structure . Ferroelectric domains in barium titanate may be observed by optical means , as the crystals are transparent and exhibit different . indices of refraction parallel and perpendicular to the tetragonal axis of a domain ...
... domain structure . Ferroelectric domains in barium titanate may be observed by optical means , as the crystals are transparent and exhibit different . indices of refraction parallel and perpendicular to the tetragonal axis of a domain ...
Page 419
... arrangement shown . = It is possible to devise domain arrangements such as ( d ) and ( e ) for which the magnetic energy is zero . Here the boundaries of the M ( gauss ) triangular prism domains ( termed " FERROMAGNETIC DOMAINS 419.
... arrangement shown . = It is possible to devise domain arrangements such as ( d ) and ( e ) for which the magnetic energy is zero . Here the boundaries of the M ( gauss ) triangular prism domains ( termed " FERROMAGNETIC DOMAINS 419.
Page 420
Charles Kittel. M ( gauss ) triangular prism domains ( termed " domains of closure " ) near the end faces of the crystal make equal angles - 45 ° -with the magnetiza- tion in the rectangular domains and with the magnetization in the ...
Charles Kittel. M ( gauss ) triangular prism domains ( termed " domains of closure " ) near the end faces of the crystal make equal angles - 45 ° -with the magnetiza- tion in the rectangular domains and with the magnetization in the ...
Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
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absorption acceptors alkali alloys approximately atoms axes axis barium titanate boundary Bragg Brillouin zone calculated chapter charge conduction band conduction electrons crystal structure cube cubic Curie point Debye density dielectric constant diffraction diffusion dipole direction discussion dislocation distribution domain effective mass elastic electric field energy equation equilibrium exciton experimental F centers factor Fermi ferroelectric ferromagnetic free electron frequency germanium given heat capacity hexagonal holes impurity interaction ionization ions lattice constant lattice point low temperatures magnetic field magnetic moment metals molecules motion nearest neighbor normal observed p-n junction paramagnetic particles phonons Phys physics plane polarizability polarization positive potential Proc resonance result room temperature rotation semiconductor Shockley shown in Fig sodium chloride solid solution space group specimen spin superconducting surface susceptibility symmetry Table theory thermal tion transistor transition unit volume vacancies valence band values vector velocity wave functions wavelength x-ray zero