Introduction to Solid State Physics |
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Page 95
The dielectric loss may be obtained from the sharpness of the tuning near
resonance . ... and here one often measures essentially the wavelength of the
microwave radiation in the specimen , obtaining the dielectric constant from the
relation ...
The dielectric loss may be obtained from the sharpness of the tuning near
resonance . ... and here one often measures essentially the wavelength of the
microwave radiation in the specimen , obtaining the dielectric constant from the
relation ...
Page 189
4 , 1948 . The value of 0 is obtained by fitting an expression of the form x = C / ( T
+ 0 ) to the susceptibility above the actual transition temperature Tc . In recent
literature the transition or Curie temperature is sometimes referred to as the Néel
...
4 , 1948 . The value of 0 is obtained by fitting an expression of the form x = C / ( T
+ 0 ) to the susceptibility above the actual transition temperature Tc . In recent
literature the transition or Curie temperature is sometimes referred to as the Néel
...
Page 218
9 , where the penetration depths are compared with those obtained by Pippard
from high frequency resistance measurements . Other values are given in Table
11 . 3 . TABLE 11 . 3 . VALUES OF THE PENETRATION DEPTH
EXTRAPOLATED ...
9 , where the penetration depths are compared with those obtained by Pippard
from high frequency resistance measurements . Other values are given in Table
11 . 3 . TABLE 11 . 3 . VALUES OF THE PENETRATION DEPTH
EXTRAPOLATED ...
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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 |