Treatise on Materials Science and TechnologyHerbert Herman |
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Page 5
... atomic meshes on both sides in parallel orientation . For the present it is adequate to regard the interfacial atomic symmetry as being quadratic with atomic spacings a and b . The model disregards the superstructures , which are ...
... atomic meshes on both sides in parallel orientation . For the present it is adequate to regard the interfacial atomic symmetry as being quadratic with atomic spacings a and b . The model disregards the superstructures , which are ...
Page 32
... atom is Ω Q = bxb , nb2 ( 3.74 ) where n is the number of atomic layers . It accordingly follows from ( 3.31 ) and ( 3.72 ) - ( 3.74 ) that 12 = nl。2 / ( 1 −σ2 ) ( 3.75 ) when there exists quadratic interfacial symmetry . Hence one ...
... atom is Ω Q = bxb , nb2 ( 3.74 ) where n is the number of atomic layers . It accordingly follows from ( 3.31 ) and ( 3.72 ) - ( 3.74 ) that 12 = nl。2 / ( 1 −σ2 ) ( 3.75 ) when there exists quadratic interfacial symmetry . Hence one ...
Page 39
... atomic centers the represent- ing shear stress ( 4.6 ) is assumed to act on the atomic planes through these centers . In principle therefore these planes are also the interfacial planes of the elastic continua . Mathematically the plane ...
... atomic centers the represent- ing shear stress ( 4.6 ) is assumed to act on the atomic planes through these centers . In principle therefore these planes are also the interfacial planes of the elastic continua . Mathematically the plane ...
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