Introduction to Solid State Physicsproblems after each chapter |
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Page 75
It is important so to arrange the terms in the series that the contributions from the
positive and negative terms nearly cancel , or else the series will not converge .
In the sodium chloride structure there are six positive ions ( the nearest neighbors
...
It is important so to arrange the terms in the series that the contributions from the
positive and negative terms nearly cancel , or else the series will not converge .
In the sodium chloride structure there are six positive ions ( the nearest neighbors
...
Page 298
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 filled
energy band behave as if endowed with a positive charge . States of this
character ...
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 filled
energy band behave as if endowed with a positive charge . States of this
character ...
Page 300
For the portion of the energy surface to the left of F the slope E / ak , is positive ;
from ( 11 . 37 ) the group velocity is ( 11 . 71 ) ve = ħ - 1 2E / aka , so that we have
a positive velocity . We see then that the velocity of the hole increases in the ...
For the portion of the energy surface to the left of F the slope E / ak , is positive ;
from ( 11 . 37 ) the group velocity is ( 11 . 71 ) ve = ħ - 1 2E / aka , so that we have
a positive velocity . We see then that the velocity of the hole increases in the ...
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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