Treatise on Materials Science and TechnologyHerbert Herman |
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Page 106
... crystal imperfec- tions on the other . For an ideal mosaic crystal , it is sufficient to determine integrated reflectivities of Bragg reflections in order to deduce the structure . Crystal imperfections normally have little influence on ...
... crystal imperfec- tions on the other . For an ideal mosaic crystal , it is sufficient to determine integrated reflectivities of Bragg reflections in order to deduce the structure . Crystal imperfections normally have little influence on ...
Page 320
... crystals sink in it . e . Flux PbO - PbF2 - B2O3 : Large optical quality crystals ( 60 g for each crystal ) of YAG and ReAG were grown with PbO - PbF2 - B2O3 as the flux ( Van Uitert et al . , 1965 ) . Y ̧Ni ̧ Ge , Fe5-2x O12 crystals ...
... crystals sink in it . e . Flux PbO - PbF2 - B2O3 : Large optical quality crystals ( 60 g for each crystal ) of YAG and ReAG were grown with PbO - PbF2 - B2O3 as the flux ( Van Uitert et al . , 1965 ) . Y ̧Ni ̧ Ge , Fe5-2x O12 crystals ...
Page 354
... crystal linewidth . For a composition of x = 0.40 and y = 0.60 , its linewidth of 2.2 Oe can be resolved into 0.58 ± 0.16 Oe for rare earth impurity , 0.22 ± 0.11 Oe for anisotropy , 0.98 ± 0.53 Oe for porosity , and 0.42 ± 0.36 Oe for ...
... crystal linewidth . For a composition of x = 0.40 and y = 0.60 , its linewidth of 2.2 Oe can be resolved into 0.58 ± 0.16 Oe for rare earth impurity , 0.22 ± 0.11 Oe for anisotropy , 0.98 ± 0.53 Oe for porosity , and 0.42 ± 0.36 Oe for ...
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