Introduction to Solid State Physics |
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Page 15
fcc lattice is shown in Fig . 1 . 8 and is a rhombohedron of volume onequarter that
of the unit cube . We may think of a bcc lattice as made up of two interpenetrating
sc lattices , and of a foc lattice as made up of four interpenetrating sc lattices .
fcc lattice is shown in Fig . 1 . 8 and is a rhombohedron of volume onequarter that
of the unit cube . We may think of a bcc lattice as made up of two interpenetrating
sc lattices , and of a foc lattice as made up of four interpenetrating sc lattices .
Page 153
The level scheme for a single electron spin is shown in Fig . 9 . 2 .
Electromagnetic radiation of frequency such that ( 9 . 24 ) hw = quoH will induce
transitions between neighboring magnetic levels according to the selection rule
amg = + 1 for ...
The level scheme for a single electron spin is shown in Fig . 9 . 2 .
Electromagnetic radiation of frequency such that ( 9 . 24 ) hw = quoH will induce
transitions between neighboring magnetic levels according to the selection rule
amg = + 1 for ...
Page 172
Charles Kittel. field at the expense of unfavorably oriented domains ; or by
rotation of the directions of magnetization toward the direction of the field . These
two methods by which the resultant magnetization may change are shown in Fig .
10 .
Charles Kittel. field at the expense of unfavorably oriented domains ; or by
rotation of the directions of magnetization toward the direction of the field . These
two methods by which the resultant magnetization may change are shown in Fig .
10 .
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Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
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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