Introduction to Solid State Physics |
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Page 96
ELECTRONIC POLARIZABILITIES The total polarizability of an atom or ion may
usually be separated into three parts : electronic , ionic , and orientational . The
electronic contribution arises from the displacement of electrons in an atom ...
ELECTRONIC POLARIZABILITIES The total polarizability of an atom or ion may
usually be separated into three parts : electronic , ionic , and orientational . The
electronic contribution arises from the displacement of electrons in an atom ...
Page 172
These two methods by which the resultant magnetization may change are shown
in Fig . 10 . 8 . Closer examination reveals that in weak fields the magnetization
changes usually proceed by means of domain boundary displacements ...
These two methods by which the resultant magnetization may change are shown
in Fig . 10 . 8 . Closer examination reveals that in weak fields the magnetization
changes usually proceed by means of domain boundary displacements ...
Page 266
9 shows that the Grüneisen relation works quite well for the metals indicated
there ; at quite low temperatures , however , departures from the TTM law are
usually observed . Reference to detailed theoretical calculations of the
conductivity of ...
9 shows that the Grüneisen relation works quite well for the metals indicated
there ; at quite low temperatures , however , departures from the TTM law are
usually observed . Reference to detailed theoretical calculations of the
conductivity of ...
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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