Introduction to Solid State Physics |
From inside the book
Results 1-3 of 24
Page 23
Writing U ( r ) dr = 4wr4p ( r ) dr as the probability that an electron lies ur
Scattering plane Fig . 1 . 16 . Calculation of the atomic scattering factor f . The
normal to the scattering plane is S . between radii r and r + dr , we have ( 1 . 11 )
sin MT dr ...
Writing U ( r ) dr = 4wr4p ( r ) dr as the probability that an electron lies ur
Scattering plane Fig . 1 . 16 . Calculation of the atomic scattering factor f . The
normal to the scattering plane is S . between radii r and r + dr , we have ( 1 . 11 )
sin MT dr ...
Page 282
73 MOBILITY IN THE PRESENCE OF IMPURITY ATOMS When relatively few
impurity atoms are present , or at high temperatures , lattice scattering will
determine the mobility . At higher impurity concentrations , electron scattering by
impurity ...
73 MOBILITY IN THE PRESENCE OF IMPURITY ATOMS When relatively few
impurity atoms are present , or at high temperatures , lattice scattering will
determine the mobility . At higher impurity concentrations , electron scattering by
impurity ...
Page 370
ELECTRICAL CONDUCTIVITY AT LOW TEMPERATURES At low temperatures
the electrons may only be scattered through small angles , so the number of
scattering processes needed to reduce the average forward momentum by a
given ...
ELECTRICAL CONDUCTIVITY AT LOW TEMPERATURES At low temperatures
the electrons may only be scattered through small angles , so the number of
scattering processes needed to reduce the average forward momentum by a
given ...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
Copyright | |
13 other sections not shown
Other editions - View all
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