Introduction to Solid State Physics |
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Page 151
... zero field splitting may be caused by electrostatic effects ( Appendix H ) , by the interaction of the magnetic moments with each other , or by nuclear interactions . The zero field splitting causes the entropy at T2 in Fig . 9.5 to be ...
... zero field splitting may be caused by electrostatic effects ( Appendix H ) , by the interaction of the magnetic moments with each other , or by nuclear interactions . The zero field splitting causes the entropy at T2 in Fig . 9.5 to be ...
Page 202
... zero resistivity p : from E = pj we see that , if p is zero while j is finite , then E must be zero and with it curl E must be zero . Therefore from Maxwell's equations ( 11.1 ) dB -c curl E dt = so that the flux through the metal ...
... zero resistivity p : from E = pj we see that , if p is zero while j is finite , then E must be zero and with it curl E must be zero . Therefore from Maxwell's equations ( 11.1 ) dB -c curl E dt = so that the flux through the metal ...
Page 363
... zero - point motion of the spin . wave system . K. THE BLOCH THEOREM We now prove that the lowest state of a quantum ... zero for the ground state . This means that at absolute zero the system cannot have a spontaneous current . Bohm has ...
... zero - point motion of the spin . wave system . K. THE BLOCH THEOREM We now prove that the lowest state of a quantum ... zero for the ground state . This means that at absolute zero the system cannot have a spontaneous current . Bohm has ...
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