Introduction to Solid State Physics |
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Page 117
... interaction energy of a dipole with the local internal electric field caused by the polarization itself . The interaction energy is ( p · E ) ; as E will be of the order of -Ps , the interaction energy is of the order of ( 3 × 10−18 ) ...
... interaction energy of a dipole with the local internal electric field caused by the polarization itself . The interaction energy is ( p · E ) ; as E will be of the order of -Ps , the interaction energy is of the order of ( 3 × 10−18 ) ...
Page 148
... interaction energy is introduced as an additional perturbatior on the system , the quenching may be partially lifted as the spin may carry some orbital moment along with it . If the sign of the spin orbit interaction favors parallel ...
... interaction energy is introduced as an additional perturbatior on the system , the quenching may be partially lifted as the spin may carry some orbital moment along with it . If the sign of the spin orbit interaction favors parallel ...
Page 196
... interactions A A , B B , and AB are all anti- ferromagnetic , but the AB interaction is usually considerably the strongest , so that the A and B lattices are individually ferromagnetic but with the magnetizations MA , MB oppositely ...
... interactions A A , B B , and AB are all anti- ferromagnetic , but the AB interaction is usually considerably the strongest , so that the A and B lattices are individually ferromagnetic but with the magnetizations MA , MB oppositely ...
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