Introduction to Solid State Physicsproblems after each chapter |
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Page 186
The interaction energy is – } ( p · E ) ; as E will be of the order of - P3 , the
interaction energy is of the order of } ( 5 X 10 - 18 ) ( 8 X 104 ) = 2 X 10 - 13 ergs .
We obtain the approximate transition temperature by setting the interaction
energy ...
The interaction energy is – } ( p · E ) ; as E will be of the order of - P3 , the
interaction energy is of the order of } ( 5 X 10 - 18 ) ( 8 X 104 ) = 2 X 10 - 13 ergs .
We obtain the approximate transition temperature by setting the interaction
energy ...
Page 220
When the spin - orbit interaction energy is introduced as an additional
perturbation on the system , the quenching may be partially lifted as the spin may
carry some orbital moment along with it . If the sign of the spin - orbit interaction
favors ...
When the spin - orbit interaction energy is introduced as an additional
perturbation on the system , the quenching may be partially lifted as the spin may
carry some orbital moment along with it . If the sign of the spin - orbit interaction
favors ...
Page 447
The exchange interactions A – A , B – B , and A - B are all antiferromagnetic . The
A - B interaction is usually considerably the strongest , so the A and B lattices are
individually ferromagnetic but with the magnetizations MA , M b oppositely ...
The exchange interactions A – A , B – B , and A - B are all antiferromagnetic . The
A - B interaction is usually considerably the strongest , so the A and B lattices are
individually ferromagnetic but with the magnetizations MA , M b oppositely ...
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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 neighbor 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