Introduction to Solid State Physicsproblems after each chapter |
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Page 158
If we are far enough away from the individual dipoles of a uniformly polarized
specimen , we may , according to an elementary transformation occurring in
electrostatic theory , calculate the field of the specimen as equal to the field of a
surface ...
If we are far enough away from the individual dipoles of a uniformly polarized
specimen , we may , according to an elementary transformation occurring in
electrostatic theory , calculate the field of the specimen as equal to the field of a
surface ...
Page 267
strike unit area of the surface will be the emission current density j , apart from a
factor representing quantum reflection effects which we neglect . Then ( 10 . 110 )
j = ! . ! Joter el - EP ) KT = 27° . / log [ 1 + e " , dp , dp , where ( P2 ? + pz ? ) / 2m )
...
strike unit area of the surface will be the emission current density j , apart from a
factor representing quantum reflection effects which we neglect . Then ( 10 . 110 )
j = ! . ! Joter el - EP ) KT = 27° . / log [ 1 + e " , dp , dp , where ( P2 ? + pz ? ) / 2m )
...
Page 326
36 for which the inscribed Fermi sphere makes contact with the Brillouin zone
surface for the foc lattice . The observed electron concentration of the ß phase (
bcc ) is close to the concentration 1 . 48 for which the inscribed Fermi sphere
makes ...
36 for which the inscribed Fermi sphere makes contact with the Brillouin zone
surface for the foc lattice . The observed electron concentration of the ß phase (
bcc ) is close to the concentration 1 . 48 for which the inscribed Fermi sphere
makes ...
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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 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