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

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Results 1-3 of 73

Page 35

This represents an increase of 15 % beyond that of the simple model

the 1 values to be the same . ... of the W ' value differs from the one adopted for

thick crystals , where the shape of the trough is

.

This represents an increase of 15 % beyond that of the simple model

**assuming**the 1 values to be the same . ... of the W ' value differs from the one adopted for

thick crystals , where the shape of the trough is

**assumed**to be the known quantity.

Page 39

The periodic potential representation ( 2.1 ) correspondingly becomes an

interfacial potential energy density V ( uc2 | 4n d ) [ 1 - cos ( 21U / C ) ] ( 4.5 )

where d , which is usually

two atomic ...

The periodic potential representation ( 2.1 ) correspondingly becomes an

interfacial potential energy density V ( uc2 | 4n d ) [ 1 - cos ( 21U / C ) ] ( 4.5 )

where d , which is usually

**assumed**to be equal to c , is the distance between thetwo atomic ...

Page 75

B. Modelt In the analysis the existence of a concentration gradient will be

the diffusion process itself and

flat .

B. Modelt In the analysis the existence of a concentration gradient will be

**assumed**. ... studied without regard to the effect of the dislocation strain fields onthe diffusion process itself and

**assuming**that initially the interface was sharp andflat .

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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