Introduction to Solid State PhysicsProblems after each chapter. |
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Page 234
... electrons of the constituent atoms of the metal are able to move about freely through the volume of the specimen . The valence electrons are responsible for the conduction of electricity by the metal , and for this reason these electrons ...
... electrons of the constituent atoms of the metal are able to move about freely through the volume of the specimen . The valence electrons are responsible for the conduction of electricity by the metal , and for this reason these electrons ...
Page 235
... electrons by the ion cores . In fact , it will be seen later that on the quantum theory the ion cores do not scatter the conduction electrons at all , as long as the ion cores are arranged in a perfectly regular array ; this is truly a ...
... electrons by the ion cores . In fact , it will be seen later that on the quantum theory the ion cores do not scatter the conduction electrons at all , as long as the ion cores are arranged in a perfectly regular array ; this is truly a ...
Page 251
... conduction electrons . On heat- ing from absolute zero every electron does not gain an energy ~ kT as happens classically , but only those electrons already within an energy range of the order of kT of the Fermi level can be excited ...
... conduction electrons . On heat- ing from absolute zero every electron does not gain an energy ~ kT as happens classically , but only those electrons already within an energy range of the order of kT of the Fermi level can be excited ...
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