Introduction to Solid State PhysicsProblems after each chapter. |
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Page 220
... spin - orbit interaction energy is introduced as an additional perturbation 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 ...
... spin - orbit interaction energy is introduced as an additional perturbation 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 ...
Page 221
... spin system chang- ing , the disorder of the spin system will look as it should at a lower temperature . When the specimen is demagnetized adiabatically , heat can flow into the spin system only from the system of lattice vibra- tions ...
... spin system chang- ing , the disorder of the spin system will look as it should at a lower temperature . When the specimen is demagnetized adiabatically , heat can flow into the spin system only from the system of lattice vibra- tions ...
Page 593
... spin wave . A drawing of a spin wave is shown in Fig . 0.1 . The energy of a spin wave is ( 0.9 ) E = Ja2 Σ | VSm2 , using ( 0.1 ) and ( 0.3 ) , taking care not to count interactions twice . Using our standing spin waves in a ...
... spin wave . A drawing of a spin wave is shown in Fig . 0.1 . The energy of a spin wave is ( 0.9 ) E = Ja2 Σ | VSm2 , using ( 0.1 ) and ( 0.3 ) , taking care not to count interactions twice . Using our standing spin waves in a ...
Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
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absorption acceptors alkali alloys approximately atoms axes axis barium titanate boundary Bragg Brillouin zone calculated chapter charge conduction band conduction electrons crystal structure cube cubic Curie point Debye density dielectric constant diffraction diffusion dipole direction discussion dislocation distribution domain effective mass elastic electric field energy equation equilibrium exciton experimental F centers factor Fermi ferroelectric ferromagnetic free electron frequency germanium given heat capacity hexagonal holes impurity interaction ionization ions lattice constant lattice point low temperatures magnetic field magnetic moment metals molecules motion nearest neighbor normal observed p-n junction paramagnetic particles phonons Phys physics plane polarizability polarization positive potential Proc resonance result room temperature rotation semiconductor Shockley shown in Fig sodium chloride solid solution space group specimen spin superconducting surface susceptibility symmetry Table theory thermal tion transistor transition unit volume vacancies valence band values vector velocity wave functions wavelength x-ray zero