Introduction to Solid State Physicsproblems after each chapter |
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Page 268
TABLE 10.8 . Work FUNCTIONS FROM PHOTOELECTRIC DATA Metal • ( ev )
Na 2.3 K 2.26 Cr 4.37 Zn 4.24 4. 19 Pt 6.2 PROBLEMS 10.1 . ( a ) Using the
boundary condition y = 0 on the surfaces of a cube of side L , find all the wave
functions ...
TABLE 10.8 . Work FUNCTIONS FROM PHOTOELECTRIC DATA Metal • ( ev )
Na 2.3 K 2.26 Cr 4.37 Zn 4.24 4. 19 Pt 6.2 PROBLEMS 10.1 . ( a ) Using the
boundary condition y = 0 on the surfaces of a cube of side L , find all the wave
functions ...
Page 274
wave . If the potential energies of y 1 and 2 differ by an amount AE we have ,
referring to Fig . 11.1 ( b ) , an energy gap of width AE . The wave function at
points A will be 42 , and the wave function above the energy gap at points B will
be 41 .
wave . If the potential energies of y 1 and 2 differ by an amount AE we have ,
referring to Fig . 11.1 ( b ) , an energy gap of width AE . The wave function at
points A will be 42 , and the wave function above the energy gap at points B will
be 41 .
Page 302
here follows the elementary approximate presentation by Weisskopf ; 15 the low
temperature theory is discussed in Appendix K. If the lattice of a metal is perfect
and there are no lattice vibrations , the electron waves pass through the lattice ...
here follows the elementary approximate presentation by Weisskopf ; 15 the low
temperature theory is discussed in Appendix K. If the lattice of a metal is perfect
and there are no lattice vibrations , the electron waves pass through the lattice ...
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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 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