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

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Page 237

To get the difference of the free energies for H2 = 0 , we therefore have to add the

field expulsion energy

AG90 + ( H , 2 / 87 ) ( 10 ) Therefore , whenever H , > H. = ( 87 | AGs0 | ) ( 11 ) AG

...

To get the difference of the free energies for H2 = 0 , we therefore have to add the

field expulsion energy

**density**H , / 81 . Thus we get for finite applied fields AG ,AG90 + ( H , 2 / 87 ) ( 10 ) Therefore , whenever H , > H. = ( 87 | AGs0 | ) ( 11 ) AG

...

Page 254

ELECTRON PROPERTIES Inasmuch as a net attractive interaction between

electrons due to the electron - phonon interaction is expected for quasi - particle

energy Ekl SWD , information about the electronic

Fermi ...

ELECTRON PROPERTIES Inasmuch as a net attractive interaction between

electrons due to the electron - phonon interaction is expected for quasi - particle

energy Ekl SWD , information about the electronic

**density**of states near theFermi ...

Page 262

with the critical current

and ( 25 ) gave rise to a great many discussions and misunderstandings , before

the situation was clarified by Josephson ( 1965 , 1966 ) and Evetts et al . ( 1968 )

.

with the critical current

**density**J. ( r ) . The physical facts underlying Eqs . ( 24 )and ( 25 ) gave rise to a great many discussions and misunderstandings , before

the situation was clarified by Josephson ( 1965 , 1966 ) and Evetts et al . ( 1968 )

.

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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