Introduction to Solid State Physics |
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Page 2
IONIC CRYSTALS In ionic crystals electrons are transferred from atoms of one
type to atoms of a second type , so that the crystal is made up of positive and
negative ions . The ions arrange themselves so that the Coulomb attraction
between ...
IONIC CRYSTALS In ionic crystals electrons are transferred from atoms of one
type to atoms of a second type , so that the crystal is made up of positive and
negative ions . The ions arrange themselves so that the Coulomb attraction
between ...
Page 29
Lattice Energy of Ionic Crystals When we speak of ionic crystals we mean
substances such as lithium fluoride and sodium ... The idealized model of an
ionic crystal supposes that the constituents are positive and negative ions
bearing charges ...
Lattice Energy of Ionic Crystals When we speak of ionic crystals we mean
substances such as lithium fluoride and sodium ... The idealized model of an
ionic crystal supposes that the constituents are positive and negative ions
bearing charges ...
Page 33
6 ) where r ; is the distance of the sth ion from the reference ion and is always to
be taken as positive . We shall first compute the value of the Madelung constant
for an infinite line of ions of alternating sign , as shown in Fig . 2 . 2 . We pick a ...
6 ) where r ; is the distance of the sth ion from the reference ion and is always to
be taken as positive . We shall first compute the value of the Madelung constant
for an infinite line of ions of alternating sign , as shown in Fig . 2 . 2 . We pick a ...
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Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
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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