Introduction to Solid State Physics |
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Page 30
In the crystal each ion is surrounded by six nearest neighbors of the opposite
charge and twelve next nearest neighbors of the same charge as the reference
ion . We suppose that the Nation carries a single positive charge , so that the ...
In the crystal each ion is surrounded by six nearest neighbors of the opposite
charge and twelve next nearest neighbors of the same charge as the reference
ion . We suppose that the Nation carries a single positive charge , so that the ...
Page 93
4 ) , while the ( + P = charge density on plate - P = polarization charge density on
dielectric surface V = Ew = Fig . 6 . 4 . Definitions of D and E ; the voltage V
across the condenser plates is E times the separation w , if we neglect the air
gaps ...
4 ) , while the ( + P = charge density on plate - P = polarization charge density on
dielectric surface V = Ew = Fig . 6 . 4 . Definitions of D and E ; the voltage V
across the condenser plates is E times the separation w , if we neglect the air
gaps ...
Page 313
We shall consider a lattice made up of ions with positive or negative charges of
the same magnitude and shall assume that ... The potential 41 is that of a lattice
with a Gaussian distribution of charge situated at each lattice point , with signs
the ...
We shall consider a lattice made up of ions with positive or negative charges of
the same magnitude and shall assume that ... The potential 41 is that of a lattice
with a Gaussian distribution of charge situated at each lattice point , with signs
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