Introduction to Solid State Physics |
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Page 11
A parallel three - dimensional net - like arrangement of points is by definition a
space lattice , provided that the environment about any particular point is the
same as about any other . With each lattice point there may be associated a
group of ...
A parallel three - dimensional net - like arrangement of points is by definition a
space lattice , provided that the environment about any particular point is the
same as about any other . With each lattice point there may be associated a
group of ...
Page 173
17 The coercive force is defined as the reverse field needed to reduce the
induction B or the magnetization M to zero , starting in a saturated condition .
Usually the definition is understood to refer to B , except in theoretical work .
When referred ...
17 The coercive force is defined as the reverse field needed to reduce the
induction B or the magnetization M to zero , starting in a saturated condition .
Usually the definition is understood to refer to B , except in theoretical work .
When referred ...
Page 306
5 We have defined the long range T / TC order parameter S so that the Fig . 15 . 6
. Long range order S ... a B on a , then ( 15 . 10 ) e r — W S = or + w ' this may be
considered an alternative but equivalent definition of S . The short range order ...
5 We have defined the long range T / TC order parameter S so that the Fig . 15 . 6
. Long range order S ... a B on a , then ( 15 . 10 ) e r — W S = or + w ' this may be
considered an alternative but equivalent definition of S . The short range order ...
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Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
Copyright | |
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alloy applied approximation atoms axes axis band boundary calculated cell chapter charge chloride condition conductivity consider constant crystal cubic defined dependence determined dielectric diffusion direction discussed dislocations displacement distance distribution domains effect elastic electric electron energy equal equation equilibrium example excitation experimental expression factor field force frequency function given gives heat holes interaction ionic ions lattice levels London magnetic magnetic field material mean measurements mechanism metals method molecules motion negative neighbor normal observed obtained parallel particles Phys physical plane polarization positive possible potential problem properties quantum range reference reflection region relation resistivity result room temperature scattering Show shown in Fig sodium solids space specimen stress structure suppose Table temperature theory thermal tion transition unit usually vacancy values volume wave zero