Treatise on Materials Science and TechnologyHerbert Herman |
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Page 124
... components , i.e. , there normally exist 3yo different phonon branches . Further , V , is a vector of 3 % components with the condition Vj Vj = 8jj ( II.77 ) Reference should be made to the textbook monograph for methods 124 W. SCHMATZ 74.
... components , i.e. , there normally exist 3yo different phonon branches . Further , V , is a vector of 3 % components with the condition Vj Vj = 8jj ( II.77 ) Reference should be made to the textbook monograph for methods 124 W. SCHMATZ 74.
Page 189
... components . The phonon line widths are of the same order of magnitude as the phonon frequency shifts relative to the pure components . In a very rough approximation one is inclined to say , the disordered state has a phonon frequency ...
... components . The phonon line widths are of the same order of magnitude as the phonon frequency shifts relative to the pure components . In a very rough approximation one is inclined to say , the disordered state has a phonon frequency ...
Page 294
... component , is for nonzero component , is for equal components , is for components equal numerically , but opposite in sign , is for a component equal to twice the heavy dot component to which it is joined , is for a component equal to ...
... component , is for nonzero component , is for equal components , is for components equal numerically , but opposite in sign , is for a component equal to twice the heavy dot component to which it is joined , is for a component equal to ...
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