Introduction to Solid State Physics |
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Page 91
Charles Kittel. principal axes parallel to the applied field , the polarization will be parallel to the applied field , as will the depolarization field E1 , which it is found may be calculated from the polarization P by a relation of ...
Charles Kittel. principal axes parallel to the applied field , the polarization will be parallel to the applied field , as will the depolarization field E1 , which it is found may be calculated from the polarization P by a relation of ...
Page 118
... parallel to a cube edge above 0 ° C , becomes parallel to a face diagonal below 0 ° C and parallel to a body diagonal below -80 ° C , as the ratios of the P , at the transition temperatures are approximately 1 : 1/2 : 1/3 . [ After ...
... parallel to a cube edge above 0 ° C , becomes parallel to a face diagonal below 0 ° C and parallel to a body diagonal below -80 ° C , as the ratios of the P , at the transition temperatures are approximately 1 : 1/2 : 1/3 . [ After ...
Page 191
... parallel to H will be , for small angles , -2XMA , and at equilibrium this is equal to but opposite H. The total magnetization component parallel to H is Μφ ( MA + MB ) $ = 2M , so that = ( 10.60 ) H = хм , or ( 10.61 ) Χι = ( T ≤ Tc ) ...
... parallel to H will be , for small angles , -2XMA , and at equilibrium this is equal to but opposite H. The total magnetization component parallel to H is Μφ ( MA + MB ) $ = 2M , so that = ( 10.60 ) H = хм , or ( 10.61 ) Χι = ( T ≤ Tc ) ...
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