Introduction to Solid State Physics |
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Results 1-3 of 88
Page 115
5 BaTiO3 perovskite 391 48 , 000 KTaO : perovskite NaTa03 perovskite KNb03
perovskite 708 NaNO3 perovskite 913 LiTa03 ilmenite 70 , 000 ( 425°C ) LiNb03
ilmenite WO : modified 220 ( ? ) perovskite a Discovered by J . Valasek , Phys .
5 BaTiO3 perovskite 391 48 , 000 KTaO : perovskite NaTa03 perovskite KNb03
perovskite 708 NaNO3 perovskite 913 LiTa03 ilmenite 70 , 000 ( 425°C ) LiNb03
ilmenite WO : modified 220 ( ? ) perovskite a Discovered by J . Valasek , Phys .
Page 131
Cohen 17 has 14 C . Kittel , Phys . Rev . 82 , 729 ( 1951 ) . 16 Kehl , Hay , and
Wahl , J . Appl . Phys . 23 , 212 ( 1952 ) ; for x - ray work on the ionic
displacements in barium titanate , see W . Kaenzig , Helv . Phys . Acta 24 , 175 (
1951 ) .
Cohen 17 has 14 C . Kittel , Phys . Rev . 82 , 729 ( 1951 ) . 16 Kehl , Hay , and
Wahl , J . Appl . Phys . 23 , 212 ( 1952 ) ; for x - ray work on the ionic
displacements in barium titanate , see W . Kaenzig , Helv . Phys . Acta 24 , 175 (
1951 ) .
Page 320
50 , 705 ( 1936 ) ; G . H . Wannier , Phys . Rev . 52 , 191 ( 1937 ) ; W . R . Heller
and A . Marcus , Phys . Rev . 84 , 809 ( 1951 ) . 16 L . Apker and E . Taft , Phys .
Rev . 79 , 964 ( 1950 ) ; 81 , 698 ( 1951 ) ; 82 , 814 ( 1951 ) ; M . H . Hebb , Phys .
50 , 705 ( 1936 ) ; G . H . Wannier , Phys . Rev . 52 , 191 ( 1937 ) ; W . R . Heller
and A . Marcus , Phys . Rev . 84 , 809 ( 1951 ) . 16 L . Apker and E . Taft , Phys .
Rev . 79 , 964 ( 1950 ) ; 81 , 698 ( 1951 ) ; 82 , 814 ( 1951 ) ; M . H . Hebb , Phys .
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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