Introduction to Solid State Physics |
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Page 251
... mass m * such that a2W / ak2 = h2 / m * . It may be shown that the motion of a wave packet in applied electric or magnetic fields is characterized by using m * as the mass . Near the top of a band m is negative , so that here the motion ...
... mass m * such that a2W / ak2 = h2 / m * . It may be shown that the motion of a wave packet in applied electric or magnetic fields is characterized by using m * as the mass . Near the top of a band m is negative , so that here the motion ...
Page 258
... mass ratio m * / m is of the order of 10 or more . Experimental values of the effective mass ratio are given in Table 13.1 . The mag- netic susceptibilities are shown in Fig . 13.6 ; it is seen that some of the transition metals have ...
... mass ratio m * / m is of the order of 10 or more . Experimental values of the effective mass ratio are given in Table 13.1 . The mag- netic susceptibilities are shown in Fig . 13.6 ; it is seen that some of the transition metals have ...
Page 377
... mass , m Planck's constant , h ( h- " bar " ) , ħ Velocity of light , c Faraday constant , F = Ne Specific charge of ... mass to electron mass Boltzmann's constant , k Bohr magneton , μB = eh / 2mc Wavelength associated with 1 ev , λo ...
... mass , m Planck's constant , h ( h- " bar " ) , ħ Velocity of light , c Faraday constant , F = Ne Specific charge of ... mass to electron mass Boltzmann's constant , k Bohr magneton , μB = eh / 2mc Wavelength associated with 1 ev , λo ...
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