Introduction to Solid State Physics |
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Page 251
Effective mass . Near the top or bottom of a band the energy is generally a
quadratic function of the wave numbers , so that by analogy with the expression
W = ( h2 / 2m ) k2 for free electrons we may define an effective mass m * such that
32W ...
Effective mass . Near the top or bottom of a band the energy is generally a
quadratic function of the wave numbers , so that by analogy with the expression
W = ( h2 / 2m ) k2 for free electrons we may define an effective mass m * such that
32W ...
Page 258
Susceptibility per gram of several transition metals . have unusually large
electronic heat capacities , suggesting that the effective mass ratio m * / m is of
the order of 10 or more . Experimental values of the effective mass ratio are given
in Table ...
Susceptibility per gram of several transition metals . have unusually large
electronic heat capacities , suggesting that the effective mass ratio m * / m is of
the order of 10 or more . Experimental values of the effective mass ratio are given
in Table ...
Page 377
Quantity Value Avogadro ' s number , L ( 6 . 025438 + 0 . 000107 ) X 1023 g mol -
1 ( phys . ) Electronic charge , e - ( 4 . 802233 + 0 . 000071 ) X 10 - 10 esu
Electron rest mass , m ( 9 . 107208 + 0 . 000246 ) X 10 - 28 grams Planck ' s
constant ...
Quantity Value Avogadro ' s number , L ( 6 . 025438 + 0 . 000107 ) X 1023 g mol -
1 ( phys . ) Electronic charge , e - ( 4 . 802233 + 0 . 000071 ) X 10 - 10 esu
Electron rest mass , m ( 9 . 107208 + 0 . 000246 ) X 10 - 28 grams Planck ' s
constant ...
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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