Introduction to Solid State Physics |
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Page 143
... level splitting scheme for one electron , with only spin angular momentum , in a magnetic field H directed along the positive z axis . Note that the Bohr magneton μв = eh / 2mc is a negative number as used here . H the energy levels are ...
... level splitting scheme for one electron , with only spin angular momentum , in a magnetic field H directed along the positive z axis . Note that the Bohr magneton μв = eh / 2mc is a negative number as used here . H the energy levels are ...
Page 144
... levels , and N = N1 N2 is the total number of atoms . The projection of the magnetic moment of the upper state along the field direction is gμB / 2 , and of the lower state is guB / 2 , so that the resultant magnetization for N atoms ...
... levels , and N = N1 N2 is the total number of atoms . The projection of the magnetic moment of the upper state along the field direction is gμB / 2 , and of the lower state is guB / 2 , so that the resultant magnetization for N atoms ...
Page 146
... Levels >> kT above the ground state may contribute to the susceptibility a term which is independent of temperature over the appropriate range . This term is known as Van 1 A multiplet is the set of levels of different J values arising ...
... Levels >> kT above the ground state may contribute to the susceptibility a term which is independent of temperature over the appropriate range . This term is known as Van 1 A multiplet is the set of levels of different J values arising ...
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