## Treatise on Materials Science and Technology, Volume 2 |

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Results 1-3 of 30

Page 184

A localized

) do = 1 ( IV.71 ) 2 02 in the case of a cubic Bravais lattice with ... It is ε = ( M. - MD

/ Mh . € has to be 0.4 in order to get a well separated from the band

A localized

**mode**with frequency w is given by g ( w ) do 2 EWL = 1 with 596 ) ( w) do = 1 ( IV.71 ) 2 02 in the case of a cubic Bravais lattice with ... It is ε = ( M. - MD

/ Mh . € has to be 0.4 in order to get a well separated from the band

**modes**.Page 189

23 where the transversal optical

between 2950 and 15 ° K. The phase transition , however ... Usually the critical

point has a special symmetry and the condensing soft

hw . ) ?

23 where the transversal optical

**mode**for KTO , shows a dramatic changebetween 2950 and 15 ° K. The phase transition , however ... Usually the critical

point has a special symmetry and the condensing soft

**mode**follows the relation (hw . ) ?

Page 193

has exactly the same rotation angle in the same direction , then the critical point

for the soft

the critical point is at R. Mainly R points have been observed . The 186 ° K phase

...

has exactly the same rotation angle in the same direction , then the critical point

for the soft

**mode**is at point M of the Brillouin zone ; if the rotation is just oppositethe critical point is at R. Mainly R points have been observed . The 186 ° K phase

...

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### Contents

Epitaxial Interfaces | 3 |

Thin Films | 15 |

Semiinfinite Overgrowths | 37 |

Copyright | |

11 other sections not shown

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### Common terms and phrases

angle anisotropy approximation assumed atoms average axis c-sites calculated cations coherent concentration condition considerations constant contribution corresponding crystal curve defect density dependence determined diffusion direction discussed dislocations displacement effect elastic elastic scattering electron energy equation et al exist experimental experiments factor field flux lines follows force function garnet given gives important increasing Inelastic Scattering interaction interface ions lattice length limit magnetic materials measured Merwe metal method misfit mode neutron normal obtained parameter phase phonon Phys plane position potential present properties range rare earth reasonable reference region relation resolution respectively sample scattering cross section shown shows single solid solution space strain stress structure substrate superconducting surface Table temperature tetrahedral theory thermal thickness transition unit values vector X-ray