Introduction to Solid State PhysicsProblems after each chapter. |
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Page 249
... zero all the levels below a certain level will be filled with elec- trons , and all levels above it will be empty of electrons . The level which divides the filled and vacant levels is known as the Fermi level at absolute zero and is ...
... zero all the levels below a certain level will be filled with elec- trons , and all levels above it will be empty of electrons . The level which divides the filled and vacant levels is known as the Fermi level at absolute zero and is ...
Page 454
... zero while j is finite , then E must be zero and with it curl E must be zero . Therefore from Maxwell's equations ( 16.1 ) dB = c curl E = dt so that the flux through the metal cannot change on cooling through the transition . The ...
... zero while j is finite , then E must be zero and with it curl E must be zero . Therefore from Maxwell's equations ( 16.1 ) dB = c curl E = dt so that the flux through the metal cannot change on cooling through the transition . The ...
Page 464
... zero resistance , as this assumption accounts directly for the persistent currents and the zero resistivity . Attempts were made to set up quantum - mechanical models which would have the property that the lowest state of the system ...
... zero resistance , as this assumption accounts directly for the persistent currents and the zero resistivity . Attempts were made to set up quantum - mechanical models which would have the property that the lowest state of the system ...
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