1979
DOI: 10.1103/physrevb.19.742
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Spontaneous recombination volumes of Frenkel defects in neutron-irradiated non-fcc metals

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Cited by 39 publications
(10 citation statements)
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“…1 is non-trivial. Defects with a wide range of concentrations can be prepared experimentally, including FP concentrations of 0.2–0.6 at.% in most metals at low temperature 31 and up to 3 at.% in graphite at room temperature 27 . Our choice of 1 at.% represents a practically achievable limit in most materials.…”
Section: Resultsmentioning
confidence: 99%
“…1 is non-trivial. Defects with a wide range of concentrations can be prepared experimentally, including FP concentrations of 0.2–0.6 at.% in most metals at low temperature 31 and up to 3 at.% in graphite at room temperature 27 . Our choice of 1 at.% represents a practically achievable limit in most materials.…”
Section: Resultsmentioning
confidence: 99%
“…[7,12,31,38,43,47,63,65,[72][73][74][75]. The data are shown in Table 2 for various metals and types of irradiation.…”
Section: Systematics Of Frenkel Pair Resistivitymentioning
confidence: 99%
“…The second group (TTB(2)) includes data for dDq=dU ð Þ j Dq¼0 obtained in Refs. [31,[73][74][75] for modified TTB spectrum and corrected as described in Ref. [7].…”
Section: Ttb Frmmentioning
confidence: 99%
“…Saturation resistivities for neutronirradiated Zr have been reported previously from four experiments: kosenbaum et al 1 give ap s » 24 nn.m for Zr irradiated at 77 K, Vialaret et al 2 report ap s * 100 nn.iu for irradiation at 24 K, while Nakagawa et al 3 and Klabunde and Coltman give values of zoo n .ai and 47 nfl.m, respectively, for irradiation at 4.5 K. It has been suggested that the large range of £p s measured (and thus of V r calculated) may originate from differences in irradiation temperature. Other possible sources for the discrepancy could be trace impurities, spectrum effects, or simply the difficulty in extrapolating the damage-rate curves.…”
Section: Introductionmentioning
confidence: 59%