Introduction to Solid State Physics |
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Page 134
DERIVATION OF THE LANGEVIN DIAMAGNETISM EQUATION The usual
derivation employs the Larmor theorem , which states that for an atom in a
magnetic field the motion of the electrons is , to the first order in H , the same as a
possible ...
DERIVATION OF THE LANGEVIN DIAMAGNETISM EQUATION The usual
derivation employs the Larmor theorem , which states that for an atom in a
magnetic field the motion of the electrons is , to the first order in H , the same as a
possible ...
Page 181
The magnetization of the crystal “ sees ” the crystal lattice through the agency of
the orbital motion of the electrons ; the spin interacts with the orbital motion by
means of the spin orbit coupling , and the orbital motion in turn interacts with the ...
The magnetization of the crystal “ sees ” the crystal lattice through the agency of
the orbital motion of the electrons ; the spin interacts with the orbital motion by
means of the spin orbit coupling , and the orbital motion in turn interacts with the ...
Page 305
The motion has been demonstrated in a beautiful experiment by Washburn and
Parker . The nature of their results is exhibited in Fig . 16 . 7b . The specimen
consisted of a bicrystal of zinc having an orientation difference of 2° . Fig . 16 . 7a
.
The motion has been demonstrated in a beautiful experiment by Washburn and
Parker . The nature of their results is exhibited in Fig . 16 . 7b . The specimen
consisted of a bicrystal of zinc having an orientation difference of 2° . Fig . 16 . 7a
.
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Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
Copyright | |
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alloy applied approximation atoms axes axis band boundary calculated cell chapter charge chloride condition conductivity consider constant crystal cubic defined dependence determined dielectric diffusion direction discussed dislocations displacement distance distribution domains effect elastic electric electron energy equal equation equilibrium example excitation experimental expression factor field force frequency function given gives heat holes interaction ionic ions lattice levels London magnetic magnetic field material mean measurements mechanism metals method molecules motion negative neighbor normal observed obtained parallel particles Phys physical plane polarization positive possible potential problem properties quantum range reference reflection region relation resistivity result room temperature scattering Show shown in Fig sodium solids space specimen stress structure suppose Table temperature theory thermal tion transition unit usually vacancy values volume wave zero