Introduction to Solid State Physics |
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The rapid rise of interest in solid state physics in recent years has suddenly
presented universities with the problem of offering adequate instruction in the
subject . It seems to me that there should be an introductory or survey course
followed by ...
The rapid rise of interest in solid state physics in recent years has suddenly
presented universities with the problem of offering adequate instruction in the
subject . It seems to me that there should be an introductory or survey course
followed by ...
Page 64
These features of the onedimensional problem are characteristic also of the
lattice vibration problems in two and three dimensions . We sometimes wish to
know the number of modes per unit range of k . We shall denote this quantity by
w ( k ) ...
These features of the onedimensional problem are characteristic also of the
lattice vibration problems in two and three dimensions . We sometimes wish to
know the number of modes per unit range of k . We shall denote this quantity by
w ( k ) ...
Page 271
... for four free valence electrons per atom . PROBLEMS 13 . ... Bryan and H . W .
B . Skinner , Phys . Rev . 45 , 370 ( 1934 ) ; review papers by Skinner are cited in
Problem 13 . 5 . 13 . 7 . Discuss the principal physical features of PROBLEMS
271.
... for four free valence electrons per atom . PROBLEMS 13 . ... Bryan and H . W .
B . Skinner , Phys . Rev . 45 , 370 ( 1934 ) ; review papers by Skinner are cited in
Problem 13 . 5 . 13 . 7 . Discuss the principal physical features of PROBLEMS
271.
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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