Introduction to Solid State Physics |
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Page 183
8 - 29 — 25 62 90 64 d , as ahapter . . . think o nisotrops For nickel , expression (
10 . 33 ) does not give a very good fit to the observations , and an expression
involving four parameters instead of two is often used , as discussed by Becker
and ...
8 - 29 — 25 62 90 64 d , as ahapter . . . think o nisotrops For nickel , expression (
10 . 33 ) does not give a very good fit to the observations , and an expression
involving four parameters instead of two is often used , as discussed by Becker
and ...
Page 282
Charles Kittel. for the equilibrium number of ionized donors . This expression
holds only when the ratio Ne / N , is « 1 . Exact values of Ne for a typical example
are given in Table 14 . 3 . At high temperatures the donors will become
completely ...
Charles Kittel. for the equilibrium number of ionized donors . This expression
holds only when the ratio Ne / N , is « 1 . Exact values of Ne for a typical example
are given in Table 14 . 3 . At high temperatures the donors will become
completely ...
Page 351
C . QUANTUM - MECHANICAL EXPRESSION FOR THE POLARIZABILITY We
compute the energy of interaction of an atomic system with an applied static
electric field and set this equal to the macroscopic expression for the energy ,
which is ...
C . QUANTUM - MECHANICAL EXPRESSION FOR THE POLARIZABILITY We
compute the energy of interaction of an atomic system with an applied static
electric field and set this equal to the macroscopic expression for the energy ,
which is ...
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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