physica status solidi (b) · 1966 · 17 citations · 23 references
Natural SciencesMaterials EngineeringMaterials ScienceMaterials CharacterizationMaterials PhysicsRadiation MeasurementDefect CharacterizationDefectsDefects In Electronic MaterialsRadiation Damage In MaterialsAnnealingDefect Evolution Under IrradiationElectrical ResistivityIrradiation ConditionsNeutron Irradiation EffectsRadiation DefectsResistivityVolume Change
Abstract Pure aluminium samples are irradiated at 4 °K in the core of the Munich Research Reactor. Measurements are then made of the release of the stored energy (Δ Q and the changes in the length (Δ l ) and electrical resistivity (Δ∂) during annealing between 4 and 300 °K. For the first annealing stage, observed between 4 and 55 °K, these measurements yield \documentclass{article}\pagestyle{empty}\begin{document}$ \frac{{\Delta Q}}{{\Delta \varrho}} = 38.3 \pm 1.3Ws/g\mu \Omega {\rm cm,}\frac{{\Delta l/l}}{{\Delta \varrho}} = 0.12 \pm 0.005\frac{\%}{{\mu \Omega {\rm cm}}}$ \end{document} . The corresponding ratios for the two other observed stages have similar values. The experimental results suggest the following values for specific properties of defects in aluminium ( E F , E i , E v being the energies of a Frenkel defect, an interstitial, and a vacancy, respectively; V F is the volume change per Frenkel defect; ∂ F , ∂ i , ∂ v are the resistivity changes per unit concentration of Frenkel defects, interstitials, and vacancies, respectively): E F = 3.4 eV; E v = 0.8 eV; E i = 2.6 eV; V F = 1.2 atomvol.; ∂ F = 340 μΩcm; ∂ v = 220 μΩcm; ∂ i = 120 μΩcm.
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Dislocation loops in quenched aluminium
P. B. Hirsch, J. Silcox, R.E. Smallman et al. · Philosophical magazine · 1958 · 339 citations
Isochronal annealing of vacancies in aluminium
C. Panseri, T. Federighi · Philosophical magazine · 1958 · 116 citations
Natural Sciences, Materials Engineering, Materials Science +13