Introduction to Solid State Physics |
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Page 261
Each zone or band is readily shown to contain 2N electronic states , as may be
seen on thinking of the bands as arising from the overlap of atomic states . If each
atom has two valence electrons , there will be a total of 2N electrons , completely
...
Each zone or band is readily shown to contain 2N electronic states , as may be
seen on thinking of the bands as arising from the overlap of atomic states . If each
atom has two valence electrons , there will be a total of 2N electrons , completely
...
Page 273
The character of the electronic band scheme leading to intrinsic conductivity is
exhibited in Fig . 14 . 1 . At absolute zero we postulate a vacant conduction band ,
separated by an energy gap W , from a filled valence band . As the temperature is
...
The character of the electronic band scheme leading to intrinsic conductivity is
exhibited in Fig . 14 . 1 . At absolute zero we postulate a vacant conduction band ,
separated by an energy gap W , from a filled valence band . As the temperature is
...
Page 275
If we suppose that the electrons in the conduction band behave as if they are free
, we may take the density of states in the conduction band as equal to that for free
electrons , with the energy referred to the bottom of the band . Thus , from ( 12 .
If we suppose that the electrons in the conduction band behave as if they are free
, we may take the density of states in the conduction band as equal to that for free
electrons , with the energy referred to the bottom of the band . Thus , from ( 12 .
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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
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 |