Introduction to Solid State PhysicsProblems after each chapter. |
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Page 553
... consider an incoherent grain boundary to be a thin slab of low - resistance material , SA thick , of diffusivity DB . They similarly consider each dislocation in a low - angle grain boundary to be a rod of low - resistivity material ...
... consider an incoherent grain boundary to be a thin slab of low - resistance material , SA thick , of diffusivity DB . They similarly consider each dislocation in a low - angle grain boundary to be a rod of low - resistivity material ...
Page 576
... considering a very small spherical cavity , just large enough to contain one molecule . If we consider this cavity real ... consider the potential such that E = -Vp . Outside the cavity the potential may be written as ( C.1 ) = - ( + Bor ) ...
... considering a very small spherical cavity , just large enough to contain one molecule . If we consider this cavity real ... consider the potential such that E = -Vp . Outside the cavity the potential may be written as ( C.1 ) = - ( + Bor ) ...
Page 581
... consider the behavior of a simple model . We consider a single electron with orbital quantum number L 1 moving about a nucleus , the whole being placed in an inhomogeneous crystalline electric field . We omit electron spin from the ...
... consider the behavior of a simple model . We consider a single electron with orbital quantum number L 1 moving about a nucleus , the whole being placed in an inhomogeneous crystalline electric field . We omit electron spin from the ...
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