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 310
11.21 drawn for the K emission band of sodium . The experimental K emission
band of lithium is shown in Fig . 11.22 . It is important to observe LiK that the
width of emission band should be a good measure of the width of the filled
portion of ...
11.21 drawn for the K emission band of sodium . The experimental K emission
band of lithium is shown in Fig . 11.22 . It is important to observe LiK that the
width of emission band should be a good measure of the width of the filled
portion of ...
Page 332
This assumption takes care of the magnetic moment and leaves 0.54 electron for
the 4s band . The separation in energy between the 3d sub - bands is a result of
the exchange interaction discussed in Chapter 15 . When the metal is heated ...
This assumption takes care of the magnetic moment and leaves 0.54 electron for
the 4s band . The separation in energy between the 3d sub - bands is a result of
the exchange interaction discussed in Chapter 15 . When the metal is heated ...
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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