Introduction to Solid State Physicsproblems after each chapter |
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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 48 band can hold two
electrons per atom ; it is shown half - filled , as copper has one valence electron ...
Schematic relationship of 4s and 3d bands in metallic copper . The 3d band
holds ten electrons per atom and is filled in copper . The 48 band can hold two
electrons per atom ; it is shown half - filled , as copper has one valence electron ...
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 .
Page 332
number in terms of the energy band model . For nickel we have to accommodate
10 ... 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 above
the ...
number in terms of the energy band model . For nickel we have to accommodate
10 ... 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 above
the ...
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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 mass material measurements metals method motion normal observed obtained parallel particles Phys physics plane polarization positive possible potential present 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