Introduction to Solid State Physicsproblems after each chapter |
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Page xiii
Quantum theory of free particles in a box . Fermi - Dirac distribution law . Absolute
zero . Low temperatures ( kT < Ep ) . Quantum theory of the heat capacity of the
electron gas . Quantum theory of spin paramagnetism . Effect of Fermi - Dirac ...
Quantum theory of free particles in a box . Fermi - Dirac distribution law . Absolute
zero . Low temperatures ( kT < Ep ) . Quantum theory of the heat capacity of the
electron gas . Quantum theory of spin paramagnetism . Effect of Fermi - Dirac ...
Page 269
... for sodium at room temperature , using the observed conductivity . 10 . 10 . *
Apply the Boltzmann transport equation to the free electron theory of
thermoelectric effects , following the treatment in the book by Seitz listed in the
references .
... for sodium at room temperature , using the observed conductivity . 10 . 10 . *
Apply the Boltzmann transport equation to the free electron theory of
thermoelectric effects , following the treatment in the book by Seitz listed in the
references .
Page 298
This situation represented a famous unsolved problem until clarified by band
theory . A positive Hall constant implies that the current is carried by positive
charges . We shall see that on band theory vacant states near the top of an
otherwise ...
This situation represented a famous unsolved problem until clarified by band
theory . A positive Hall constant implies that the current is carried by positive
charges . We shall see that on band theory vacant states near the top of an
otherwise ...
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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