Introduction to Solid State PhysicsProblems after each chapter. |
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Page 273
... wave vector . In Fig . 11.2 ( a ) we have indicated the gen- eral nature of the variation of the electrostatic potential energy of a conduction electron in the field of the positive ion cores of a monatomic linear lattice . We expect ...
... wave vector . In Fig . 11.2 ( a ) we have indicated the gen- eral nature of the variation of the electrostatic potential energy of a conduction electron in the field of the positive ion cores of a monatomic linear lattice . We expect ...
Page 274
... waves eik , then in form- ing a solution of the wave equation as the boundaries are approached and Bragg reflection becomes imminent the wave eik gradually is sup- plemented by an increasing admixture of the wave eilk- ( 2a ) ...
... waves eik , then in form- ing a solution of the wave equation as the boundaries are approached and Bragg reflection becomes imminent the wave eik gradually is sup- plemented by an increasing admixture of the wave eilk- ( 2a ) ...
Page 284
... wave vector in approximately the same way as for a free electron while at the same time the wave function may be quite unlike a plane wave , but may pile up charge on the positive ion cores much as in the isolated atom . In the last ...
... wave vector in approximately the same way as for a free electron while at the same time the wave function may be quite unlike a plane wave , but may pile up charge on the positive ion cores much as in the isolated atom . In the last ...
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 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 resonance result room temperature rotation semiconductor Shockley shown in Fig sodium chloride solid solution space group specimen spin superconducting surface susceptibility symmetry Table theory thermal tion transistor transition unit volume vacancies valence band values vector velocity wave functions wavelength x-ray zero