Introduction to Solid State Physics |
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Page 25
15 ) , F ( hkl ) = fs , where S is called the geometrical structure factor and is given
by ( 1 . 17 ) S = ei27 ( hu ; + kv ; + lw ; ) A body - centered cubic structure of
identical atoms has atoms at 000 and } } } . We find ( 1 . 18 ) S = 1 + eir ( h + k + i )
.
15 ) , F ( hkl ) = fs , where S is called the geometrical structure factor and is given
by ( 1 . 17 ) S = ei27 ( hu ; + kv ; + lw ; ) A body - centered cubic structure of
identical atoms has atoms at 000 and } } } . We find ( 1 . 18 ) S = 1 + eir ( h + k + i )
.
Page 35
747558 which has been worked out for the sodium chloride structure by the
Ewald method . The Ewald method is derived and discussed in Appendix B .
Values of Madelung constants for many different crystal structures are tabulated
by ...
747558 which has been worked out for the sodium chloride structure by the
Ewald method . The Ewald method is derived and discussed in Appendix B .
Values of Madelung constants for many different crystal structures are tabulated
by ...
Page 116
The structure is cubic , with Ba2 + ions at the cube corners , 02 - ions at the face
centers , and a Ti4 + ion at the body center . Below the Curie temperature the
structure is slightly deformed with respect to that described here . The prototype ...
The structure is cubic , with Ba2 + ions at the cube corners , 02 - ions at the face
centers , and a Ti4 + ion at the body center . Below the Curie temperature the
structure is slightly deformed with respect to that described here . The prototype ...
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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 |