Introduction to Solid State Physicsproblems after each chapter |
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Page 207
DIAMAGNETISM Substances with a negative magnetic susceptibility are called
diamagnetic . The magnetic susceptibility per unit volume is defined as . 1 x = II /
H , where M is the magnetic moment per unit volume , or the magnetization , and
...
DIAMAGNETISM Substances with a negative magnetic susceptibility are called
diamagnetic . The magnetic susceptibility per unit volume is defined as . 1 x = II /
H , where M is the magnetic moment per unit volume , or the magnetization , and
...
Page 220
netic field in the z direction the orbital contribution to the magnetic moment is
proportional to the expectation value of Lz , and so the orbital magnetic moment
is quenched if the mechanical moment L , is quenched . When the spin - orbit ...
netic field in the z direction the orbital contribution to the magnetic moment is
proportional to the expectation value of Lz , and so the orbital magnetic moment
is quenched if the mechanical moment L , is quenched . When the spin - orbit ...
Page 414
15 FERROMAGNETIC DOMAINS17 At temperatures well below the Curie point
the electronic magnetic moments of a ferromagnetic specimen are essentially all
lined up , when regarded on a microscopic scale . Yet , looking at a specimen as
...
15 FERROMAGNETIC DOMAINS17 At temperatures well below the Curie point
the electronic magnetic moments of a ferromagnetic specimen are essentially all
lined up , when regarded on a microscopic scale . Yet , looking at a specimen as
...
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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