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 gμÅ / 2 , and of the lower state is gMB / 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 gμÅ / 2 , and of the lower state is gMB / 2 , so that the resultant magnetization for N atoms ...
Page 146
... levels are considered . The full theoretical expression for the susceptibility as a function of temperature when higher states are to be considered may be quite complicated . In Appendix F we consider two limiting cases , when the level ...
... levels are considered . The full theoretical expression for the susceptibility as a function of temperature when higher states are to be considered may be quite complicated . In Appendix F we consider two limiting cases , when the level ...
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