Introduction to Solid State Physicsproblems after each chapter |
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Page 139
If the energy were propagated directly through the specimen without deflection , then the expression for the thermal flux would not depend on the temperature gradient , but only on the difference in temperature AT between the ends of ...
If the energy were propagated directly through the specimen without deflection , then the expression for the thermal flux would not depend on the temperature gradient , but only on the difference in temperature AT between the ends of ...
Page 431
... introduced in Problem 15.2 : 2 B ( 15.34 ) λι00 30u C12 1 B2 λι11 3 C44 Experimental values are : 1100 X 106 du X 106 B , X 106 ergs / cm2 B , X 106 ergs / cm3 Fe 19.5 -18.8 -29 64 Ni -46 - 25 62 90 For nickel , expression ( 15.33 ) ...
... introduced in Problem 15.2 : 2 B ( 15.34 ) λι00 30u C12 1 B2 λι11 3 C44 Experimental values are : 1100 X 106 du X 106 B , X 106 ergs / cm2 B , X 106 ergs / cm3 Fe 19.5 -18.8 -29 64 Ni -46 - 25 62 90 For nickel , expression ( 15.33 ) ...
Page 534
Derive an expression for the orbital g - factor of a simple exciton composed of an electron of effective mass me and a hole of effective mass ma ; show that the orbital magnetic moment vanishes if me = mh . 18.2 .
Derive an expression for the orbital g - factor of a simple exciton composed of an electron of effective mass me and a hole of effective mass ma ; show that the orbital magnetic moment vanishes if me = mh . 18.2 .
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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