Introduction to Solid State Physicsproblems after each chapter |
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Page 249
The ground level and the first excited level can hold a maximum of 2 + 12 14
electrons , and at absolute zero the 14 states will ... Proceeding in this way we
gradually move up the energy levels of the system until all the available electrons
are ...
The ground level and the first excited level can hold a maximum of 2 + 12 14
electrons , and at absolute zero the 14 states will ... Proceeding in this way we
gradually move up the energy levels of the system until all the available electrons
are ...
Page 275
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 six hydrogen atoms in a ...
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 six hydrogen atoms in a ...
Page 505
Energy levels of an exciton whose center of mass is at rest . ... When one
considers the translational motion of the center of mass of the exciton it is
apparent that there is a continuum of levels associated with each exciton level
shown here .
Energy levels of an exciton whose center of mass is at rest . ... When one
considers the translational motion of the center of mass of the exciton it is
apparent that there is a continuum of levels associated with each exciton level
shown here .
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Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
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alloys applied approximately associated atoms axis band boundary calculated cell chapter charge concentration condition conductivity consider constant crystal cubic density dependence determined dielectric diffusion direction discussion dislocation distribution domain effect elastic electric electron elements energy equal equation equilibrium experimental expression factor field force frequency function germanium give given heat capacity hexagonal holes important impurity increase interaction ionic ions lattice levels London magnetic magnetic field mass material measurements metals method motion normal observed obtained parallel particles Phys physics plane polarization positive possible potential problem properties range reference reflection region relation resistivity result room temperature rotation shown in Fig simple solid solution space space group specimen structure surface symmetry Table temperature theory thermal tion transition unit usually values vector volume wave zero zone