Treatise on Materials Science and TechnologyHerbert Herman |
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Page 141
... sample geometry . sample area F of thickness D and forward scattering - N has to be replaced by N → No e DFD ( III.21 ) Assuming this geometry and similar beam attenuation fo and f1 we can give a simple expression for the intensity ...
... sample geometry . sample area F of thickness D and forward scattering - N has to be replaced by N → No e DFD ( III.21 ) Assuming this geometry and similar beam attenuation fo and f1 we can give a simple expression for the intensity ...
Page 142
... Sample thicknesses used are given in the table . The table demonstrates that K TABLE IV -1 RATIO OF COUNTING RATES Z1 , N / Z1 , x , NEUTRONS VS. X - RAYS " Thickness Element DN ... SAMPLE ( TRANSMISSION ) dill aill SAMPLE 142 W. SCHMATZ.
... Sample thicknesses used are given in the table . The table demonstrates that K TABLE IV -1 RATIO OF COUNTING RATES Z1 , N / Z1 , x , NEUTRONS VS. X - RAYS " Thickness Element DN ... SAMPLE ( TRANSMISSION ) dill aill SAMPLE 142 W. SCHMATZ.
Page 353
... samples , the linewidth was 0.1 Oe for best polish and 10 Oe for 20 μm grit polish ( LeCraw et al . , 1958 ) . In polycrystalline YIG samples , the sample of 99 % density had a maximum AH of 15 Oe , and the sample of 79 % had a maximum ...
... samples , the linewidth was 0.1 Oe for best polish and 10 Oe for 20 μm grit polish ( LeCraw et al . , 1958 ) . In polycrystalline YIG samples , the sample of 99 % density had a maximum AH of 15 Oe , and the sample of 79 % had a maximum ...
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 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