Treatise on Materials Science and TechnologyHerbert Herman |
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Results 1-3 of 16
Page 174
... interstitials can be assumed and lattice parameter measurements of Wagner et al . ( 1970 ) a specific resistivity of 390 ± 80 μN cm per Frenkel pair and a relative volume change of A / 2 , 1.9 ± 0.3 per interstitial in aluminum has been ...
... interstitials can be assumed and lattice parameter measurements of Wagner et al . ( 1970 ) a specific resistivity of 390 ± 80 μN cm per Frenkel pair and a relative volume change of A / 2 , 1.9 ± 0.3 per interstitial in aluminum has been ...
Page 221
... interstitials their distortion ( about 100 to 1000 interstitials per cluster ) is strong enough to produce a significant ... interstitial clusters produced by fast neutron irradiation in copper single crystals of extremely low initial ...
... interstitials their distortion ( about 100 to 1000 interstitials per cluster ) is strong enough to produce a significant ... interstitial clusters produced by fast neutron irradiation in copper single crystals of extremely low initial ...
Page 222
... interstitial loops have in the average larger size than vacancy loops . From this it follows that under the experimental conditions , the contribution of interstitial loops is predominant . This explains the asymmetry observed by Thomas ...
... interstitial loops have in the average larger size than vacancy loops . From this it follows that under the experimental conditions , the contribution of interstitial loops is predominant . This explains the asymmetry observed by Thomas ...
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