Introduction to Solid State Physics |
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Page 63
The actual atomic nature of the line affects the propagation when k becomes
comparable with km . π / α Fig . 4 . 2 . Plot of frequency w vs . wave number k for a
monatomic linear lattice . The phase velocity is a function of the wave number
and ...
The actual atomic nature of the line affects the propagation when k becomes
comparable with km . π / α Fig . 4 . 2 . Plot of frequency w vs . wave number k for a
monatomic linear lattice . The phase velocity is a function of the wave number
and ...
Page 106
DIPOLE RELAXATION AND DIELECTRIC LOSSES The principal part of the
difference between the low frequency dielectric constant and the high frequency
dielectric constant as measured by the square of the optical refractive index may
be ...
DIPOLE RELAXATION AND DIELECTRIC LOSSES The principal part of the
difference between the low frequency dielectric constant and the high frequency
dielectric constant as measured by the square of the optical refractive index may
be ...
Page 111
For light of frequency w show that the classical expression for the polarizability of
a single electron bound to a nucleus is e / m a wo ? - w2 where wo is the
resonance frequency of the electron . 6 . 4 . Show that the polarizability of a
conducting ...
For light of frequency w show that the classical expression for the polarizability of
a single electron bound to a nucleus is e / m a wo ? - w2 where wo is the
resonance frequency of the electron . 6 . 4 . Show that the polarizability of a
conducting ...
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Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
Copyright | |
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Common terms and phrases
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
Bibliographic information
| Title | Introduction to Solid State Physics Wiley series on the science and technology of materials |
| Author | Charles Kittel |
| Edition | 2 |
| Publisher | Wiley, 1953 |
| Original from | the University of Michigan |
| Digitized | 21 Nov 2007 |
| Length | 396 pages |
| Export Citation | BiBTeX EndNote RefMan |