Introduction to Solid State Physicsproblems after each chapter |
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Page 108
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 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 unit range of k . We shall denote this quantity by w ( k ) ...
Page 338
To be more precise , the transition temperature marks the disappearance of long range order over many interatomic distances , but some short range 1 Order S - - - Tc Absolute temperature Fig . 12.24 . Long range ( S ) and short range ...
To be more precise , the transition temperature marks the disappearance of long range order over many interatomic distances , but some short range 1 Order S - - - Tc Absolute temperature Fig . 12.24 . Long range ( S ) and short range ...
Page 343
This transcendental equation for S may be solved graphically , and it 1.0 Long range order S 0.5 1.0 0.5 T / Tc Fig . 12.28 . Long range order S vs. temperature for an AB alloy . gives the smoothly decreasing curve shown in Fig .
This transcendental equation for S may be solved graphically , and it 1.0 Long range order S 0.5 1.0 0.5 T / Tc Fig . 12.28 . Long range order S vs. temperature for an AB alloy . gives the smoothly decreasing curve shown in Fig .
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Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
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alloys applied approximately associated atoms axis band boundary calculated cell chapter charge concentration condition conductivity consider constant crystal cubic density dependence determined dielectric diffusion direction discussion dislocation distribution domain effect elastic electric electron elements energy equal equation equilibrium experimental expression factor field force frequency function germanium give given heat capacity hexagonal holes important impurity increase interaction ionic ions lattice levels London magnetic magnetic field mass material measurements metals method motion normal observed obtained parallel particles Phys physics plane polarization positive possible potential present problem properties range reference reflection region relation resistivity result room temperature rotation shown in Fig simple solid solution space space group specimen structure surface symmetry Table temperature theory thermal tion transition unit usually values vector volume wave zero zone