Introduction to Solid State Physicsproblems after each chapter |
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Page 277
Effect of orbital degeneracy on band structure . We have then the important result
that a band formed from L / a atoms contains 2L / a states . If each atom
contributes one valence electron to the band , the band will be half full and the
solid will ...
Effect of orbital degeneracy on band structure . We have then the important result
that a band formed from L / a atoms contains 2L / a states . If each atom
contributes one valence electron to the band , the band will be half full and the
solid will ...
Page 330
Schematic relationship of 4s and 3d bands in metallic copper . The 3d band
holds ten electrons per atom and is filled in copper . The 4s band can hold two
electrons per atom ; it is shown half - filled , as copper has one valence electron
outside ...
Schematic relationship of 4s and 3d bands in metallic copper . The 3d band
holds ten electrons per atom and is filled in copper . The 4s band can hold two
electrons per atom ; it is shown half - filled , as copper has one valence electron
outside ...
Page 331
There is a considerable energy gap between the top of the d band and the Fermi
surface lying in the s band . It is useful for later applications to show the bands
divided in two halves , one half for each orientation of the electron spin . In Fig .
There is a considerable energy gap between the top of the d band and the Fermi
surface lying in the s band . It is useful for later applications to show the bands
divided in two halves , one half for each orientation of the electron spin . In Fig .
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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 neighbor 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