Introduction to Solid State Physicsproblems after each chapter |
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Page 124
The Debye model , shortly to be discussed , gives a satisfactory account of the T°
variation . ... The Einstein model does , however , give a fairly good
representation of the drop in heat capacity at low temperatures , provided that we
make an ...
The Debye model , shortly to be discussed , gives a satisfactory account of the T°
variation . ... The Einstein model does , however , give a fairly good
representation of the drop in heat capacity at low temperatures , provided that we
make an ...
Page 142
50 ) ki + k , = k3 , two phonons 1 and 2 colliding to give rise to a single phonon 3 .
Collisions of this type do not ... This type of collision , which Peierls called an
Umklapp process , gives rise to thermal resistance . The energy associated with ...
50 ) ki + k , = k3 , two phonons 1 and 2 colliding to give rise to a single phonon 3 .
Collisions of this type do not ... This type of collision , which Peierls called an
Umklapp process , gives rise to thermal resistance . The energy associated with ...
Page 475
He suggests that any model of superconductivity which gives correctly the
thermodynamical properties of the superconducting state will most likely give the
Meissner effect . More recent determinations of the heat capacity of
superconductors at ...
He suggests that any model of superconductivity which gives correctly the
thermodynamical properties of the superconducting state will most likely give the
Meissner effect . More recent determinations of the heat capacity of
superconductors at ...
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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