Treatise on Materials Science and TechnologyHerbert Herman |
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Page 92
... 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 fact that the tangential forces ... Normal Forces Appendix B Normal Forces Model.
... 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 fact that the tangential forces ... Normal Forces Appendix B Normal Forces Model.
Page 236
... normal areas cannot be discontinuous . Changes in the density n , of Cooper pairs cannot occur within less than the ... normal and superconducting area . Let AGso be the difference between the specific free energy of a metal in the ...
... normal areas cannot be discontinuous . Changes in the density n , of Cooper pairs cannot occur within less than the ... normal and superconducting area . Let AGso be the difference between the specific free energy of a metal in the ...
Page 238
... normal state at H. with the possibility of super- cooling the normal state ( nucleation problems because of the positive surface energy ) . Figure 4a shows a typical magnetization curve . ( a ) ( b ) -4πMA ( c ) Hc -4πMA TYPE I TYPE II ...
... normal state at H. with the possibility of super- cooling the normal state ( nucleation problems because of the positive surface energy ) . Figure 4a shows a typical magnetization curve . ( a ) ( b ) -4πMA ( c ) Hc -4πMA TYPE I TYPE II ...
Contents
Epitaxial Interfaces | 3 |
Thin Films | 15 |
Semiinfinite Overgrowths | 37 |
Copyright | |
11 other sections not shown
Common terms and phrases
a-site alloy Amer anisotropy Appl approximation atoms average axis B₁ Bragg Bragg reflections c-sites calculated cations coefficients coherent compounds concentration configuration constant Cooper pairs curve Debye-Waller factor defect density dependence discussed displacement elastic electron energy epitaxial equation experimental factor ferrimagnetic field film flux lines function garnet garnet structure GdIG Geller IAEA impurity Inelastic Scattering interaction interface iron garnets k₁ lattice constant lattice parameter Lett magnetic magnetocrystalline anisotropy measured Merwe method misfit misfit dislocations mode neutron scattering normal obtained overgrowth phase phonon Phys plane potential Proc properties rare earth rare earth ions reciprocal lattice resolution sample scattering cross section shown in Fig single crystal small angle solid strain stress sublattice substrate superconducting surface symmetry Table temperature tetrahedral thermal thickness transition metal values vector X-ray YGaG