Introduction to Solid State Physics |
From inside the book
Results 1-3 of 40
Page 33
We pick a Reference ion + O + c + b + c + + Rok Fig . 2 . 2 . Line of ions of
alternating signs with distance Ro between ions . negative ion as reference ion ,
and let Ro denote the distance between adjacent ions . We have h = [ + 2 + + sło
do + .
We pick a Reference ion + O + c + b + c + + Rok Fig . 2 . 2 . Line of ions of
alternating signs with distance Ro between ions . negative ion as reference ion ,
and let Ro denote the distance between adjacent ions . We have h = [ + 2 + + sło
do + .
Page 313
... HALIDE CRYSTALS Name of Center or Band Presumed Origin Excess
electron near negative ion vacancy Two excess electrons near negative ion
vacancy Electron hole near positive ion vacancyt Added H - ions in negative ion
vacancy F2 ...
... HALIDE CRYSTALS Name of Center or Band Presumed Origin Excess
electron near negative ion vacancy Two excess electrons near negative ion
vacancy Electron hole near positive ion vacancyt Added H - ions in negative ion
vacancy F2 ...
Page 314
A negative ion vacancy in an otherwise periodic lattice behaves like a positive
charge , so an electron moving about a negative ... We identify an F - center with
an electron bound to a negative ion vacancy , the electron being provided by the
...
A negative ion vacancy in an otherwise periodic lattice behaves like a positive
charge , so an electron moving about a negative ... We identify an F - center with
an electron bound to a negative ion vacancy , the electron being provided by the
...
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