Introduction to Solid State Physicsproblems after each chapter |
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Page 139
41 ) defining the conductivity implies that the process of thermal energy transfer is
a random process . The energy does not simply enter one end of the specimen
and proceed directly in a straight path to the other end , but the energy diffuses ...
41 ) defining the conductivity implies that the process of thermal energy transfer is
a random process . The energy does not simply enter one end of the specimen
and proceed directly in a straight path to the other end , but the energy diffuses ...
Page 348
electrical conductivity , as shown in Fig . 13 . 2 . At temperatures below the
intrinsic range the electrical properties are controlled by impurities , and here we
speak of impurity conductivity or extrinsic conductivity . Vacant conduction band ...
electrical conductivity , as shown in Fig . 13 . 2 . At temperatures below the
intrinsic range the electrical properties are controlled by impurities , and here we
speak of impurity conductivity or extrinsic conductivity . Vacant conduction band ...
Page 380
It has been found that the effect of irradiation in germanium is dominated by the
acceptors produced , so that it is possible to convert the conductivity type of an n -
type specimen to p - type by a low concentration ( ~ 1 : 10 " , depending on the ...
It has been found that the effect of irradiation in germanium is dominated by the
acceptors produced , so that it is possible to convert the conductivity type of an n -
type specimen to p - type by a low concentration ( ~ 1 : 10 " , depending on the ...
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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 neighbor normal observed obtained parallel particles Phys physics plane polarization positive possible potential 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