Introduction to Solid State Physics |
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Page 179
... particle : the reason is that we must rotate the magnetization over the energy hump corresponding to a direction of hard magnetization . The coercive force of fine iron particles is expected theoretically to be about 250 oersteds on the ...
... particle : the reason is that we must rotate the magnetization over the energy hump corresponding to a direction of hard magnetization . The coercive force of fine iron particles is expected theoretically to be about 250 oersteds on the ...
Page 208
... particles . The diamagnetic susceptibility of small particles is less than that of bulk superconductors . A large mercury sphere ( Fig . 11.4 ) exhibits an effective volume susceptibility of xo - 3 / 8π , whereas Shoenberg9 finds x / xo ...
... particles . The diamagnetic susceptibility of small particles is less than that of bulk superconductors . A large mercury sphere ( Fig . 11.4 ) exhibits an effective volume susceptibility of xo - 3 / 8π , whereas Shoenberg9 finds x / xo ...
Page 310
... particles is of the order of 25 to 50 lattice spacings . An alloy in which the precipitate particles are visible under an optical microscope is generally thoroughly over - aged . Mott and Nabarro have developed a dislocation theory of ...
... particles is of the order of 25 to 50 lattice spacings . An alloy in which the precipitate particles are visible under an optical microscope is generally thoroughly over - aged . Mott and Nabarro have developed a dislocation theory of ...
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