Introduction to Solid State Physics |
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Page 58
( See Problem 3 . 7 . ) For example , the value of the anisotropy constant A
defined by ( 3 . 31 ) is 18 . 7 for beta - brass ( bcc ) and only 4 . 0 for a - brass ( fcc
) . Thermal vibration amplitudes in the [ 110 ] direction should accordingly be very
large ...
( See Problem 3 . 7 . ) For example , the value of the anisotropy constant A
defined by ( 3 . 31 ) is 18 . 7 for beta - brass ( bcc ) and only 4 . 0 for a - brass ( fcc
) . Thermal vibration amplitudes in the [ 110 ] direction should accordingly be very
large ...
Page 249
A good example is the distinction between a metal and an insulator : the free
electron model cannot help us understand this difference , but the band theory
which we are about to discuss makes quite useful statements about the
difference .
A good example is the distinction between a metal and an insulator : the free
electron model cannot help us understand this difference , but the band theory
which we are about to discuss makes quite useful statements about the
difference .
Page 282
Exact values of Ne for a typical example are given in Table 14 . 3 . At high
temperatures the donors will become completely ionized , so that the
concentration of electrons in the conduction band will ultimately , as T is
increased , be dominated ...
Exact values of Ne for a typical example are given in Table 14 . 3 . At high
temperatures the donors will become completely ionized , so that the
concentration of electrons in the conduction band will ultimately , as T is
increased , be dominated ...
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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 |