Introduction to Solid State Physics |
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Page 244
in electron - phonon collisions will be equal to rep as just estimated . Comparing
Tep with tpp , we see that under the conditions specified phonons in a metal may
have considerably shorter relaxation times than phonons in a dielectric solid .
in electron - phonon collisions will be equal to rep as just estimated . Comparing
Tep with tpp , we see that under the conditions specified phonons in a metal may
have considerably shorter relaxation times than phonons in a dielectric solid .
Page 249
Band Theory of Metals The free electron theory of metals developed in the
preceding chapter gives us a good deal of insight into certain of the physical
properties of metals , yet there are other properties for which the free electron
theory is ...
Band Theory of Metals The free electron theory of metals developed in the
preceding chapter gives us a good deal of insight into certain of the physical
properties of metals , yet there are other properties for which the free electron
theory is ...
Page 270
SUBSTITUTIONAL ALLOYS It is possible to vary the electron concentration of a
metal by alloying with elements of higher or lower valence . A number of
interesting effects directly related to band theory have been found in this way .
The Hume ...
SUBSTITUTIONAL ALLOYS It is possible to vary the electron concentration of a
metal by alloying with elements of higher or lower valence . A number of
interesting effects directly related to band theory have been found in this way .
The Hume ...
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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