Introduction to Solid State Physicsproblems after each chapter |
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Page 255
The value of Ep is determined by ( 10.51 ) and depends on the temperature , but for kT / EF « 1 it can be shown that Ef ( T ) is closely equal to its value at 0 ° K . At any temperature f has the value for E = Ep . The distribution is ...
The value of Ep is determined by ( 10.51 ) and depends on the temperature , but for kT / EF « 1 it can be shown that Ef ( T ) is closely equal to its value at 0 ° K . At any temperature f has the value for E = Ep . The distribution is ...
Page 351
Values of the energy gap determined for a number of substances are given in Table 13.1 . Many of the values were determined from the slope of plots of log o vs. 1 / T ; some of the other values were determined from the long wavelength ...
Values of the energy gap determined for a number of substances are given in Table 13.1 . Many of the values were determined from the slope of plots of log o vs. 1 / T ; some of the other values were determined from the long wavelength ...
Page 488
It is possible to compare values of the diffusion constant determined directly by this method with values determined from observed conductivities with the use of the Einstein relation . It is found that the two sets of values do not ...
It is possible to compare values of the diffusion constant determined directly by this method with values determined from observed conductivities with the use of the Einstein relation . It is found that the two sets of values do not ...
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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