Introduction to Solid State Physics |
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Page 134
Diamagnetism Substances with a negative magnetic susceptibility are called
diamagnetic . The magnetic susceptibility per unit volume is defined as x = M / H ,
where M is the magnetic moment per unit volume , or the magnetization , and H is
...
Diamagnetism Substances with a negative magnetic susceptibility are called
diamagnetic . The magnetic susceptibility per unit volume is defined as x = M / H ,
where M is the magnetic moment per unit volume , or the magnetization , and H is
...
Page 148
The magnetic moment of a state is given by the average value of the magnetic
moment operator MB ( L + 2S ) over the state . For a magnetic field in the 2
direction the orbital contribution to the magnetic moment is proportional to the ...
The magnetic moment of a state is given by the average value of the magnetic
moment operator MB ( L + 2S ) over the state . For a magnetic field in the 2
direction the orbital contribution to the magnetic moment is proportional to the ...
Page 149
magnetic with respect to protons , has been measured at very low temperatures
by Laserew and Schubnikow , who found results consistent with the known
magnitude of the proton magnetic moment . This is the only static nuclear
susceptibility ...
magnetic with respect to protons , has been measured at very low temperatures
by Laserew and Schubnikow , who found results consistent with the known
magnitude of the proton magnetic moment . This is the only static nuclear
susceptibility ...
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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