Treatise on Materials Science and TechnologyHerbert Herman |
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Page 13
... addition at 2 , where there is no change in f . 2 B AB SUBSTRATE Fig . 6. Diagram representing a monolayer B on a substrate A. The dotted rectangles indicate two possible positions for the addition of new material . It appears plausible ...
... addition at 2 , where there is no change in f . 2 B AB SUBSTRATE Fig . 6. Diagram representing a monolayer B on a substrate A. The dotted rectangles indicate two possible positions for the addition of new material . It appears plausible ...
Page 94
... addition replaces cx / p by its Fourier representation ∞ cx / p = −2 ( c / p ) Σ ( −1 ) " m ̄1 sinmx ; p / 2 < x < p / 2 ( B.19 ) identities , in which the coefficients of the trigonometric functions can be com- pared , are obtained ...
... addition replaces cx / p by its Fourier representation ∞ cx / p = −2 ( c / p ) Σ ( −1 ) " m ̄1 sinmx ; p / 2 < x < p / 2 ( B.19 ) identities , in which the coefficients of the trigonometric functions can be com- pared , are obtained ...
Page 243
... addition , there are other classes of inter- metallic compounds ( reviewed by Roberts , 1967 ) that have high T's , i.e. , the D8 ( σ - phase ) , the A - 12 ( α - Mn ) , the C - 14 ( MgZn2 ) , the C - 15 ( Cu , Mg ) Laves phase ...
... addition , there are other classes of inter- metallic compounds ( reviewed by Roberts , 1967 ) that have high T's , i.e. , the D8 ( σ - phase ) , the A - 12 ( α - Mn ) , the C - 14 ( MgZn2 ) , the C - 15 ( Cu , Mg ) Laves phase ...
Contents
Epitaxial Interfaces | 3 |
Thin Films | 15 |
Semiinfinite Overgrowths | 37 |
Copyright | |
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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 R₁ 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 thermal thickness transition metal values vector X-ray YGaG νμ ΦΩ