Introduction to Solid State Physics |
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Page 135
4 ) for a distribution of charge which on the average is spherically symmetrical ,
so that x2 = y2 = 7 ? . Then the diamagnetic susceptibility per unit volume is , if N
is the number of atoms per unit volume , ( 8 . 5 ) X = - Ze ' N _ 6mc2 " , which is
the ...
4 ) for a distribution of charge which on the average is spherically symmetrical ,
so that x2 = y2 = 7 ? . Then the diamagnetic susceptibility per unit volume is , if N
is the number of atoms per unit volume , ( 8 . 5 ) X = - Ze ' N _ 6mc2 " , which is
the ...
Page 227
Sketch of the Fermi - Dirac distribution function , for absolute zero and for a low
temperature . The region over which the distribution is affected by temperature is
of the order of KT in width . energetically accessible , and we therefore have in
the ...
Sketch of the Fermi - Dirac distribution function , for absolute zero and for a low
temperature . The region over which the distribution is affected by temperature is
of the order of KT in width . energetically accessible , and we therefore have in
the ...
Page 313
The potential 41 is that of a lattice with a Gaussian distribution of charge situated
at each lattice point , with signs the same as those of the real lattice . According to
the definition of the Madelung constant , the charge distribution on the ...
The potential 41 is that of a lattice with a Gaussian distribution of charge situated
at each lattice point , with signs the same as those of the real lattice . According to
the definition of the Madelung constant , the charge distribution on the ...
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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