Introduction to Solid State Physicsproblems after each chapter |
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Page 149
impure metals or in disordered alloys the phonon contribution may be
comparable with the electron contribution . Collisions between electrons and
phonons are of great importance . At room temperature the relaxation time of
phonon - phonon ...
impure metals or in disordered alloys the phonon contribution may be
comparable with the electron contribution . Collisions between electrons and
phonons are of great importance . At room temperature the relaxation time of
phonon - phonon ...
Page 234
Electron. Model. of. Metals. It is possible to understand a number of important
physical properties of some metals , in particular the simple monovalent metals ,
in terms of the free electron model . According to this model the valence electrons
of ...
Electron. Model. of. Metals. It is possible to understand a number of important
physical properties of some metals , in particular the simple monovalent metals ,
in terms of the free electron model . According to this model the valence electrons
of ...
Page 244
It is evident when we try to determine the consequences of the Pauli principle for
the conduction electrons of a metal that we ... For the present purpose the most
important fact about the free electron is that there is a wave associated with it , of
...
It is evident when we try to determine the consequences of the Pauli principle for
the conduction electrons of a metal that we ... For the present purpose the most
important fact about the free electron is that there is a wave associated with it , of
...
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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 axes 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 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