1976
DOI: 10.1143/jpsj.41.1584
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Quenched-in Vacancies in Aluminium

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Cited by 37 publications
(3 citation statements)
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“…Kimura, Kimura and Hasiguti(6) calculated B1 to be 0.2eV, assuming the formation energy of a vacancy in pure aluminum to be 0.76eV. Recent quenching experiments give the formation energy to be 0.70eV (7). If a smaller value is taken for the formation energy, the resulting binding energy B1 will be smaller.…”
mentioning
confidence: 99%
“…Kimura, Kimura and Hasiguti(6) calculated B1 to be 0.2eV, assuming the formation energy of a vacancy in pure aluminum to be 0.76eV. Recent quenching experiments give the formation energy to be 0.70eV (7). If a smaller value is taken for the formation energy, the resulting binding energy B1 will be smaller.…”
mentioning
confidence: 99%
“…The annealing at 350 C and the successive furnace-cooling removes excess vacancies, secondary defects and strains on and after the quenching; this annealed-out condition was adopted as a reference of the resistivity of the specimen. Normalization by dividing by R A can cancel out the effect of change in the size factor 19) of the specimen. For magnesium, the oxidation and sublimation of the surface are particularly worrisome.…”
Section: Resultsmentioning
confidence: 99%
“…Figure 3 shows d q corrected by 4t 1 /2 (nV m) with a magni® ed scale for the time axis up to 6 h in ® gure 2. The saturated value of d q is about 45 nV m. The equilibrium concentration of vacancies at 320 ë C is about 6´10 -6 in fractional terms, and the contribution to the resistivity increase is about 66 nV m using 11 mV m per atomic fraction as the speci® c electrical resistivity of vacancy (Furukawa et al 1976). The saturated value of ® gure 3 is smaller than 66 nV m. However, it should be noted that some of the vacancies were generated before the temperature attained 320 ë C, because the heating rate of this temperature rise was 60 ë C h -1 .…”
mentioning
confidence: 99%