Introduction to Solid State Physicsproblems after each chapter |
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Page 83
There are in general six orders and eight combinations of sign , making forty -
eight equivalent positions . If one of the n's is zero , there are twenty - four
equivalent positions . If two n's are equal in magnitude but different from zero ,
there are ...
There are in general six orders and eight combinations of sign , making forty -
eight equivalent positions . If one of the n's is zero , there are twenty - four
equivalent positions . If two n's are equal in magnitude but different from zero ,
there are ...
Page 180
Note : If the applied field is in the x direction , then the x component of the field of
the nucleus at the displaced position of the electron orbit must be equal to the
applied field . The correct quantum - mechanical result is larger than this by the ...
Note : If the applied field is in the x direction , then the x component of the field of
the nucleus at the displaced position of the electron orbit must be equal to the
applied field . The correct quantum - mechanical result is larger than this by the ...
Page 341
When S = 0 , each lattice contains equal numbers of A and B atoms and there is
no long range order . We consider now that part of the internal energy associated
with AA , AB , and BB nearest neighbor bond energies , with the ultimate object ...
When S = 0 , each lattice contains equal numbers of A and B atoms and there is
no long range order . We consider now that part of the internal energy associated
with AA , AB , and BB nearest neighbor bond energies , with the ultimate object ...
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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