Introduction to Solid State Physicsproblems after each chapter |
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Page 234
10 Free Electron Model of Metals 1 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 ...
10 Free Electron Model of Metals 1 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 ...
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
...
Page 526
The mode of operation of the system is as follows : ( 1 ) Light is absorbed
producing a free hole and electron leading to conductivity . ( 2 ) The hole and
electron move about in their respective bands , and eventually the hole migrates
near an ...
The mode of operation of the system is as follows : ( 1 ) Light is absorbed
producing a free hole and electron leading to conductivity . ( 2 ) The hole and
electron move about in their respective bands , and eventually the hole migrates
near an ...
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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