Introduction to Solid State PhysicsProblems after each chapter. |
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Page 268
... wave functions having the same energy ? 10.2 . Repeat the work of Problem 10.1 , but use periodic boundary conditions . 10.3 . We may obtain time - dependent wave functions by multiplying a solution -iEt / h of the wave equation of ...
... wave functions having the same energy ? 10.2 . Repeat the work of Problem 10.1 , but use periodic boundary conditions . 10.3 . We may obtain time - dependent wave functions by multiplying a solution -iEt / h of the wave equation of ...
Page 274
... wave functions at values of k far removed from the Brillouin zone boundaries / a may be represented by plane waves eik , then in form- ing a solution of the wave equation as the boundaries are approached and Bragg reflection becomes ...
... wave functions at values of k far removed from the Brillouin zone boundaries / a may be represented by plane waves eik , then in form- ing a solution of the wave equation as the boundaries are approached and Bragg reflection becomes ...
Page 284
Charles Kittel. WAVE FUNCTIONS FOR ZERO WAVE VECTOR It may appear to the reader that there is a certain inconsistency ... wave vector in approximately the same way as for a free electron while at the same time the wave function may be ...
Charles Kittel. WAVE FUNCTIONS FOR ZERO WAVE VECTOR It may appear to the reader that there is a certain inconsistency ... wave vector in approximately the same way as for a free electron while at the same time the wave function may be ...
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