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

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Page 126

important : ( 1 ) Both scattering cross sections are proportional to ke - 2W ; ( 2 )

the coherent one -

lattice points because it is proportional to won ' , which tends to infinity for a ...

important : ( 1 ) Both scattering cross sections are proportional to ke - 2W ; ( 2 )

the coherent one -

**phonon**scattering cross section is very high near reciprocallattice points because it is proportional to won ' , which tends to infinity for a ...

Page 189

the counterpart to the Bragg reflection , then the “ diffuse ” one -

scattering cross section is the counterpart to the elastic disorder cross section as

in Eq . ( 46 ) . Of course if the displacement term sp ( K ) is put equal to zero , a

random ...

the counterpart to the Bragg reflection , then the “ diffuse ” one -

**phonon**scattering cross section is the counterpart to the elastic disorder cross section as

in Eq . ( 46 ) . Of course if the displacement term sp ( K ) is put equal to zero , a

random ...

Page 248

In 1968 McMillan calculated the transition temperature of strongcoupled

superconductors as a function of the electron -

coupling constants . He noted that the electron -

depends primarily ...

In 1968 McMillan calculated the transition temperature of strongcoupled

superconductors as a function of the electron -

**phonon**and electronelectroncoupling constants . He noted that the electron -

**phonon**coupling constantdepends primarily ...

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### Contents

Epitaxial Interfaces | 3 |

Thin Films | 15 |

Semiinfinite Overgrowths | 52 |

Copyright | |

10 other sections not shown

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### Common terms and phrases

angle anisotropy approximation assumed atoms average axis c-site calculated cations coherent compounds concentration condition considerations constants contribution corresponding crystal curve decreases defect density dependence determined diffusion direction discussed dislocations displacement effect elastic elastic scattering electron energy equation et al experimental experiments factor field flux flux lines follows force function garnets given gives important impurity increases interaction interface ions lattice limit magnetic materials measured Merwe metal method misfit mode neutron normal observed obtained optical parameter phase phonon Phys plane position potential present processes properties range reference region 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 wave X-ray