Introduction to Solid State PhysicsProblems after each chapter. |
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Page 249
... 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 denoted by Ep ( 0 ) . There is considerable interest in knowing the value of the Fermi ...
... 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 denoted by Ep ( 0 ) . There is considerable interest in knowing the value of the Fermi ...
Page 275
Charles Kittel. arated energy levels are formed for each level of the isolated atom . For N atoms , N levels are formed for each level of the isolated atom , and these N levels will be associated with one or more bands . The results for ...
Charles Kittel. arated energy levels are formed for each level of the isolated atom . For N atoms , N levels are formed for each level of the isolated atom , and these N levels will be associated with one or more bands . The results for ...
Page 387
... levels are equal , there is no longer a net flow of electrons , and equilibrium obtains . liol lioleV / kT liol E ... levels here are brought into coincidence in part by electrons flowing from donor impurity levels in the semiconductor ...
... levels are equal , there is no longer a net flow of electrons , and equilibrium obtains . liol lioleV / kT liol E ... levels here are brought into coincidence in part by electrons flowing from donor impurity levels in the semiconductor ...
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