Introduction to Solid State Physics |
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Page 301
... vector called the Burgers vector . In regions where d is not parallel to the surface this relative displace- ment will either produce a gap or cause the two halves to overlap . In these cases material is either added to fill the gap or ...
... vector called the Burgers vector . In regions where d is not parallel to the surface this relative displace- ment will either produce a gap or cause the two halves to overlap . In these cases material is either added to fill the gap or ...
Page 317
... vector d . If the crystal is subjected to a shear stress σ on the upper and lower faces in the direction of slip , show by considering energy balance that the force acting on the dislocation is F do per unit length . 16.2 . Consider a ...
... vector d . If the crystal is subjected to a shear stress σ on the upper and lower faces in the direction of slip , show by considering energy balance that the force acting on the dislocation is F do per unit length . 16.2 . Consider a ...
Page 311
... vector r * ( hkl ) to the point ( h , k , l ) of the reciprocal lattice is normal to the ( hkl ) plane of the crystal lattice . ( ii ) The length of the vector r * ( hkl ) is equal to the reciprocal of the spacing of the planes ( hkl ) ...
... vector r * ( hkl ) to the point ( h , k , l ) of the reciprocal lattice is normal to the ( hkl ) plane of the crystal lattice . ( ii ) The length of the vector r * ( hkl ) is equal to the reciprocal of the spacing of the planes ( hkl ) ...
Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
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absorption alkali alloy anisotropy antiferromagnetic approximately atoms axes axis Bardeen barium titanate boundary calculated charge coefficient conduction band cube Curie point Debye density diamagnetic dielectric constant diffraction diffusion dipole direction discussed dislocation displacement domains effect elastic electric field energy entropy equation equilibrium experimental F-centers factor Fermi ferroelectric ferromagnetic free electron frequency given heat capacity holes impurity interaction ionic crystals ionized ions lattice constant lattice points London low temperatures magnetic field magnetic moment metals molecules motion nearest neighbor normal observed optical orbital parallel paramagnetic particles perovskite phonons Phys physical plane polarizability polarization positive potassium potassium chloride potential Proc quantum resonance result room temperature scattering Seitz shear Shockley shown in Fig single crystal sodium chloride solids specimen spin strain stress superconducting surface susceptibility symmetry Table theory thermal tion transition unit volume vacancy valence values vector velocity wave functions x-ray zero