Introduction to Solid State Physicsproblems after each chapter |
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Page 235
We imagine that the electrons are moving around in a random way , with a velocity distribution appropriate to a condition of thermal equilibrium at temperature T. In the absence of an applied electric field the average or drift velocity ...
We imagine that the electrons are moving around in a random way , with a velocity distribution appropriate to a condition of thermal equilibrium at temperature T. In the absence of an applied electric field the average or drift velocity ...
Page 236
or , if vp ( 0 ) is the initial drift velocity in the non - equilibrium distribution , the approach to equilibrium is described by the appropriate solution of ( 10.3 ) : ( 10.4 ) Vo ( t ) Vp ( 0 ) e - t / . We have thus arranged things ...
or , if vp ( 0 ) is the initial drift velocity in the non - equilibrium distribution , the approach to equilibrium is described by the appropriate solution of ( 10.3 ) : ( 10.4 ) Vo ( t ) Vp ( 0 ) e - t / . We have thus arranged things ...
Page 366
LIFETIME AND RECOMBINATION It is possible in semiconductors to obtain departures from the thermal equilibrium concentrations of electrons and holes in several ways : by injecting carriers into the sample through a metal contact or by ...
LIFETIME AND RECOMBINATION It is possible in semiconductors to obtain departures from the thermal equilibrium concentrations of electrons and holes in several ways : by injecting carriers into the sample through a metal contact or by ...
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Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
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alloys applied approximately associated atoms axis band boundary calculated cell chapter charge concentration condition conductivity consider constant crystal cubic density dependence determined dielectric diffusion direction discussion dislocation distribution domain effect elastic electric electron elements energy equal equation equilibrium experimental expression factor field force frequency function germanium give given heat capacity hexagonal holes important impurity increase interaction ionic ions lattice levels London magnetic magnetic field mass material measurements metals method motion normal observed obtained parallel particles Phys physics plane polarization positive possible potential present problem properties range reference reflection region relation resistivity result room temperature rotation shown in Fig simple solid solution space space group specimen structure surface symmetry Table temperature theory thermal tion transition unit usually values vector volume wave zero zone