Introduction to Solid State PhysicsProblems after each chapter. |
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Page 157
... electric field and the local electric field acting on an atom . The inter- action of the local field with the atom determines the polarization , yet the local field may itself be a function of the polarization . We then discuss the electric ...
... electric field and the local electric field acting on an atom . The inter- action of the local field with the atom determines the polarization , yet the local field may itself be a function of the polarization . We then discuss the electric ...
Page 182
... electric field of the maximum intensity which it is possible to apply without causing electrical breakdown of the crystal . We are often able to observe the spontaneous moment in these substances only when they are heated , as raising ...
... electric field of the maximum intensity which it is possible to apply without causing electrical breakdown of the crystal . We are often able to observe the spontaneous moment in these substances only when they are heated , as raising ...
Page 236
... electric field . The equa- tion of motion ( 10.5 ) has the solution ( 10.6 ) MVD = eE VD ( t ) = VD ( 0 ) + eEt / m , which does not give a steady state of the type described by Ohm's law . With a finite relaxation time the equation of ...
... electric field . The equa- tion of motion ( 10.5 ) has the solution ( 10.6 ) MVD = eE VD ( t ) = VD ( 0 ) + eEt / m , which does not give a steady state of the type described by Ohm's law . With a finite relaxation time the equation of ...
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 levels 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 region resonance result room temperature rotation semiconductor Shockley shown in Fig sodium chloride solid solution space group specimen spin superconducting surface susceptibility symmetry Table theory tion transition unit volume vacancies valence band values vector velocity wave functions wavelength x-ray zero