Introduction to Solid State Physicsproblems after each chapter |
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Page 131
It is reasonable to suppose that only those lattice modes having ħw < KT will be
excited to any appreciable extent at a low temperature T and , further , the
excitation of these modes will be approximately classical — that is , each mode
defined ...
It is reasonable to suppose that only those lattice modes having ħw < KT will be
excited to any appreciable extent at a low temperature T and , further , the
excitation of these modes will be approximately classical — that is , each mode
defined ...
Page 141
... temperatures Peierls finds A approximately proportional to e - 0 / 27 , where is
the Debye temperature . This relation has been approximately verified in an
appropriate temperature range by Berman , Simon , and Wilks , 12 as shown in
Fig .
... temperatures Peierls finds A approximately proportional to e - 0 / 27 , where is
the Debye temperature . This relation has been approximately verified in an
appropriate temperature range by Berman , Simon , and Wilks , 12 as shown in
Fig .
Page 419
is reduced ( because of the reduced spatial extension of the field ) to
approximately 1 / N of the magnetic energy of the saturated configuration ( a ) .
The subdivision process continues until the energy required to establish an
additional ...
is reduced ( because of the reduced spatial extension of the field ) to
approximately 1 / N of the magnetic energy of the saturated configuration ( a ) .
The subdivision process continues until the energy required to establish an
additional ...
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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