Introduction to Solid State Physics |
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Page 254
The allowed αα values of the energy W are given by those ranges of a = ( 2mW /
h2 ] % for which the function lies between + 1 and - 1 . ( After Kronig and Penney
... values of aa are allowed for which the left side falls in this range . The allowed
...
The allowed αα values of the energy W are given by those ranges of a = ( 2mW /
h2 ] % for which the function lies between + 1 and - 1 . ( After Kronig and Penney
... values of aa are allowed for which the left side falls in this range . The allowed
...
Page 306
8 ) , finding 4NSV + 2NKTS = 0 , so that the transition temperature Long range
order S is ( 15 . 9 ) To = – 2V / k . 1 . 0 LONG AND SHORT RANGE ORDER 0 . 5
We have defined the long range T / Tc order parameter s so that the Fig . 15 . 6 .
8 ) , finding 4NSV + 2NKTS = 0 , so that the transition temperature Long range
order S is ( 15 . 9 ) To = – 2V / k . 1 . 0 LONG AND SHORT RANGE ORDER 0 . 5
We have defined the long range T / Tc order parameter s so that the Fig . 15 . 6 .
Page 306
8 ) , finding 4NSV + 2NkTS = 0 , so that the transition temperature Long range
order S ( 15 . 9 ) To = – 2V / k . 1 . 0 LONG AND SHORT RANGE ORDER 0 . 5 We
have defined the long range T / TC order parameter S so that the Fig . 15 . 6 .
8 ) , finding 4NSV + 2NkTS = 0 , so that the transition temperature Long range
order S ( 15 . 9 ) To = – 2V / k . 1 . 0 LONG AND SHORT RANGE ORDER 0 . 5 We
have defined the long range T / TC order parameter S so that the Fig . 15 . 6 .
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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