Introduction to Solid State Physics |
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The existence of powerful theoretical methods and concepts applicable to a wide
range of problems has been an ... The major problem in writing this book has
been to conform to reasonable limitations on the length , in keeping with the spirit
...
The existence of powerful theoretical methods and concepts applicable to a wide
range of problems has been an ... The major problem in writing this book has
been to conform to reasonable limitations on the length , in keeping with the spirit
...
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 67
VIBRATIONS OF TWO - AND THREE - DIMENSIONAL LATTICES There is
usually no particular problem in setting up the equations of motion , analogous to
( 4 . 6 ) , for two - and three - dimensional lattices . The equation of motions in
three ...
VIBRATIONS OF TWO - AND THREE - DIMENSIONAL LATTICES There is
usually no particular problem in setting up the equations of motion , analogous to
( 4 . 6 ) , for two - and three - dimensional lattices . The equation of motions in
three ...
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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