Introduction to Solid State Physics |
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Page 137
... susceptibility ( 8.9 ) XM = Le2 6mc2 Σ r2 + 2 L 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 the excited state n , and ...
... susceptibility ( 8.9 ) XM = Le2 6mc2 Σ r2 + 2 L 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 the excited state n , and ...
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 3 9.6 . Making rough calculations ...
... 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 3 9.6 . Making rough calculations ...
Page 188
... susceptibility vs. temperature curve . The transition is also marked by anomalies in the heat capacity and thermal expansion coefficient . Paramagnetism Ferromagnetism M Susceptibility X = Χ Antiferromagnetism Χ Complex behavior 0 T 0 ...
... susceptibility vs. temperature curve . The transition is also marked by anomalies in the heat capacity and thermal expansion coefficient . Paramagnetism Ferromagnetism M Susceptibility X = Χ Antiferromagnetism Χ Complex behavior 0 T 0 ...
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