Introduction to Solid State Physicsproblems after each chapter |
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Page 159
The constant N is known as the depolarization factor ; it is precisely the same as
the demagnetization factor , and its value depends on the axial 1 . 0 DTTTT N / 47
4 5 6 Fig . 7 . 2 . Demagnetization factor N parallel to the figure axis of ellipsoids ...
The constant N is known as the depolarization factor ; it is precisely the same as
the demagnetization factor , and its value depends on the axial 1 . 0 DTTTT N / 47
4 5 6 Fig . 7 . 2 . Demagnetization factor N parallel to the figure axis of ellipsoids ...
Page 237
We expect the charge transported to be proportional to the charge density Ne ;
the factor em enters because the acceleration in a given electric field is
proportional to e and inversely proportional to the mass m ; the time + describes
the free ...
We expect the charge transported to be proportional to the charge density Ne ;
the factor em enters because the acceleration in a given electric field is
proportional to e and inversely proportional to the mass m ; the time + describes
the free ...
Page 615
Q factor , 179 cyclotron resonance , 374 Quenching of orbital moment , 219 , 581
R bands , 496 R centers , 495 Radiation damage , 379 Radii of ions , 81 , 82 , 83
Rare earth ions , paramagnetism , 216 Rate - grown junctions , 390 Rational ...
Q factor , 179 cyclotron resonance , 374 Quenching of orbital moment , 219 , 581
R bands , 496 R centers , 495 Radiation damage , 379 Radii of ions , 81 , 82 , 83
Rare earth ions , paramagnetism , 216 Rate - grown junctions , 390 Rational ...
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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