Introduction to Solid State Physics |
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Page 137
... susceptibility ( 8.9 ) = XM Le2 6mc2 Σ r2 + 2 L Σ | ( n│μz | 0 ) | 2 W n - - Wo where L is the Avogadro number , ( n | u2 | 0 ) is the matrix element of the z component of the orbital magnetic moment connecting the ground state with ...
... susceptibility ( 8.9 ) = XM Le2 6mc2 Σ r2 + 2 L Σ | ( n│μz | 0 ) | 2 W n - - Wo where L is the Avogadro number , ( n | u2 | 0 ) is the matrix element of the z component of the orbital magnetic moment connecting the ground state with ...
Page 159
... susceptibility . Actual paramagnetic salts may exhibit quite large anisotropies in the susceptibility , amounting , for example , to 30 % in Co ( NH4 ) 2 ( SO4 ) 2-6H2O . = 0 ) at 2 ° K of 1 cm3 9.6 . Making rough calculations , compare ...
... susceptibility . Actual paramagnetic salts may exhibit quite large anisotropies in the susceptibility , amounting , for example , to 30 % in Co ( NH4 ) 2 ( SO4 ) 2-6H2O . = 0 ) at 2 ° K of 1 cm3 9.6 . Making rough calculations , compare ...
Page 188
... susceptibility vs. temperature curve . The transition is also marked by anomalies in the heat capacity and thermal expansion coefficient . Paramagnetism Susceptibility X = M Ferromagnetism Χ Antiferromagnetism Χ Complex behavior 1 T Tc ...
... susceptibility vs. temperature curve . The transition is also marked by anomalies in the heat capacity and thermal expansion coefficient . Paramagnetism Susceptibility X = M Ferromagnetism Χ Antiferromagnetism Χ Complex behavior 1 T Tc ...
Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
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absorption alkali halides alkali metal alloy anisotropy antiferromagnetic approximation 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 entropy equation equilibrium experimental F-center factor Fermi ferroelectric ferromagnetic free electron frequency given heat capacity holes impurity interaction interstitial ionic crystals ionized lattice constant lattice points London low temperatures magnetic field magnetic moment molecules motion nearest neighbor normal observed orbital p-n junctions parallel paramagnetic particles perovskite phonons Phys physical plane polarizability polarization positive potassium chloride potential Proc quantum range order region resonance result room temperature scattering Seitz semiconductor Shockley shown in Fig single crystal sodium chloride solids specimen spin superconducting susceptibility symmetry Table theory thermal tion unit volume valence values vector velocity wave functions x-ray zero