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

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Page 129

91 ) In practice , the magnetization M is often given instead of the magnetic

induction B . Fortunately the Fourier transform of the magnetic

potential contains M in a simple form . In magnetostatics we have B ( r ) = H ( r ) +

41M ( r ) ...

91 ) In practice , the magnetization M is often given instead of the magnetic

induction B . Fortunately the Fourier transform of the magnetic

**interaction**potential contains M in a simple form . In magnetostatics we have B ( r ) = H ( r ) +

41M ( r ) ...

Page 254

ELECTRON PROPERTIES Inasmuch as a net attractive

electrons due to the electron - phonon

energy & SOD , information about the electronic density of states near the Fermi ...

ELECTRON PROPERTIES Inasmuch as a net attractive

**interaction**betweenelectrons due to the electron - phonon

**interaction**is expected for quasi - particleenergy & SOD , information about the electronic density of states near the Fermi ...

Page 268

The maximum of the order parameter between the flux lines is proportional to ( 1

– B / B . 2 ) ( de Gennes , 1966 ) , which explains the B dependence , since all

min .

The maximum of the order parameter between the flux lines is proportional to ( 1

– B / B . 2 ) ( de Gennes , 1966 ) , which explains the B dependence , since all

**interaction**models should give an**interaction**proportional to | Y ? Imax - | Y ? /min .

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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