Introduction to Solid State Physicsproblems after each chapter |
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Page 139
where Q is the flux of thermal energy ( energy transmitted across unit area per
unit time ) ; K is often expressed in units cal ... If the energy were propagated
directly through the specimen without deflection , then the expression for the
thermal ...
where Q is the flux of thermal energy ( energy transmitted across unit area per
unit time ) ; K is often expressed in units cal ... If the energy were propagated
directly through the specimen without deflection , then the expression for the
thermal ...
Page 534
Derive an expression for the orbital g - factor of an exciton composed of an
electron of effective mass me and a hole of effective mass mn ; show that the
orbital magnetic moment vanishes if me = mh . 18.2 . Does an exciton in a triplet
spin state ...
Derive an expression for the orbital g - factor of an exciton composed of an
electron of effective mass me and a hole of effective mass mn ; show that the
orbital magnetic moment vanishes if me = mh . 18.2 . Does an exciton in a triplet
spin state ...
Page 575
hwij E ; – E ; Therefore α - which is the expression to which ( 7.16 ) reduces when
w = 0. The association of the polarizability with the second order perturbation
energy of a single atomic level i depends for its validity on the condition ħwij >>
kT ' ...
hwij E ; – E ; Therefore α - which is the expression to which ( 7.16 ) reduces when
w = 0. The association of the polarizability with the second order perturbation
energy of a single atomic level i depends for its validity on the condition ħwij >>
kT ' ...
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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