Treatise on Materials Science and Technology, Volume 2 |
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Page 92
Appendix B . Normal Forces 1 . Model The assumption that the energy
contribution of the normal forces ( 2 . 14 ) is small needs justification ( van der
Merwe , 1963a ) . Recall that these are the forces which come about as a
consequence of the ...
Appendix B . Normal Forces 1 . Model The assumption that the energy
contribution of the normal forces ( 2 . 14 ) is small needs justification ( van der
Merwe , 1963a ) . Recall that these are the forces which come about as a
consequence of the ...
Page 236
difference in free energy between the superconducting and normal states . At
absolute zero the thermodynamic critical field H . ( O ) is given by H . ( 0 ) 2 / 81 =
1 / 2N ( 0 ) 42 ( 6 ) The critical field falls off with increasing temperature ...
difference in free energy between the superconducting and normal states . At
absolute zero the thermodynamic critical field H . ( O ) is given by H . ( 0 ) 2 / 81 =
1 / 2N ( 0 ) 42 ( 6 ) The critical field falls off with increasing temperature ...
Page 238
This yields type I behavior with sharp transitions between the superconductive
and the normal state at H . with the possibility of supercooling the normal state (
nucleation problems because of the positive surface energy ) . Figure 4a shows a
...
This yields type I behavior with sharp transitions between the superconductive
and the normal state at H . with the possibility of supercooling the normal state (
nucleation problems because of the positive surface energy ) . Figure 4a shows a
...
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Contents
Epitaxial Interfaces | 3 |
Thin Films | 15 |
Semiinfinite Overgrowths | 52 |
Copyright | |
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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