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

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Results 1-3 of 35

Page 92

14 ) thus

possible to solve the elastic problem with this extra boundary condition , for the

unrealistic parabolic interfacial potential ( 2 . 4 ) . By inspection of ( 2 . 4 ) , ( 4 .

14 ) thus

**becomes**Pzz ( 0 , x ) = [ 2u / ( 1 – 20 ) ] ( W / d ) ( B . 1 ) It has only beenpossible to solve the elastic problem with this extra boundary condition , for the

unrealistic parabolic interfacial potential ( 2 . 4 ) . By inspection of ( 2 . 4 ) , ( 4 .

Page 240

At a field H . 1 it

complete analogy to Eq . ( 10 ) , H . 1 can be expressed in terms of the free

energy per length of a flux line E . ( for H = 0 ) and the reduction in magnetic field

energy – P ...

At a field H . 1 it

**becomes**energetically favorable to produce flux lines . Incomplete analogy to Eq . ( 10 ) , H . 1 can be expressed in terms of the free

energy per length of a flux line E . ( for H = 0 ) and the reduction in magnetic field

energy – P ...

Page 255

For higher To materials , as the coherence length of the superconducting

electrons

the surface properties . Thus , the tunneling results for the A - 15 compounds are

...

For higher To materials , as the coherence length of the superconducting

electrons

**becomes**smaller , the tunneling results**become**more dependent onthe surface properties . Thus , the tunneling results for the A - 15 compounds are

...

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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