Introduction to Solid State Physics |
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Page 70
We note that the region of k - space for which solutions are defined is a square of
side approximately a / a ; this region is called the first Brillouin zone . Show that
the k values marking the boundary are associated with the maximum wavelength
...
We note that the region of k - space for which solutions are defined is a square of
side approximately a / a ; this region is called the first Brillouin zone . Show that
the k values marking the boundary are associated with the maximum wavelength
...
Page 294
neutralize the space charge of the donor ions , while similarly the holes
contributed by the acceptor ions will be found chiefly in the p - region . It is not
possible for the electrons and holes to remain separated in this way unless an
electric field ...
neutralize the space charge of the donor ions , while similarly the holes
contributed by the acceptor ions will be found chiefly in the p - region . It is not
possible for the electrons and holes to remain separated in this way unless an
electric field ...
Page 297
manium at the junctions between regions of n - type and p - type conductivity . ...
as shown in the figure ; therefore electrons in the collector region are not
encouraged to move to the base region ; similarly holes are held in the base
region .
manium at the junctions between regions of n - type and p - type conductivity . ...
as shown in the figure ; therefore electrons in the collector region are not
encouraged to move to the base region ; similarly holes are held in the base
region .
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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