Introduction to Solid State Physics |
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Page 100
This type of polarization was first discussed by Debye ( 1912 ) , who showed that
by assuming that molecules could have permanent dipole moments one could
explain the high dielectric constant of water , alcohol , and similar liquids , and
the ...
This type of polarization was first discussed by Debye ( 1912 ) , who showed that
by assuming that molecules could have permanent dipole moments one could
explain the high dielectric constant of water , alcohol , and similar liquids , and
the ...
Page 320
We have discussed phonons in Chapters 4 and 5 ; electrons and holes in
Chapter 14 ; excitons are discussed below ; vacant lattice sites and interstitial
atoms earlier in the present chapter ; foreign atoms in Chapter 14 and the present
chapter ...
We have discussed phonons in Chapters 4 and 5 ; electrons and holes in
Chapter 14 ; excitons are discussed below ; vacant lattice sites and interstitial
atoms earlier in the present chapter ; foreign atoms in Chapter 14 and the present
chapter ...
Page 320
We have discussed phonons in Chapters 4 and 5 ; electrons and holes in
Chapter 14 ; excitons are discussed below ; vacant lattice sites and interstitial
atoms earlier in the present chapter ; foreign atoms in Chapter 14 and the present
chapter ...
We have discussed phonons in Chapters 4 and 5 ; electrons and holes in
Chapter 14 ; excitons are discussed below ; vacant lattice sites and interstitial
atoms earlier in the present chapter ; foreign atoms in Chapter 14 and the present
chapter ...
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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