2006
DOI: 10.1016/j.radmeas.2005.02.009
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A Monte-Carlo calculation of the size distribution of latent alpha-recoil tracks in phlogopite: Implications for the recoil-track dating method

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Cited by 12 publications
(6 citation statements)
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“…As they grow-for example, during the eight successive alpha-recoil events during the complete radioactive decay chain of 238 U to 206 Pb-alpharecoil tracks typically "zigzag" through their host material (Figure 4(a)), ∼30-50 nm in new random directions with each successive alpha-recoil event (e.g., Figure 3 in Jonckheere and Gögen [131]; Table 1 in Stübner and Jonckheere [132]), resulting in a final composite cluster of radiation damage measuring about 120 nm across (e.g., estimates for the mean diameter of alpha-recoil tracks derived from the complete decay of 238 U to stable 206 Pb in micas range from ∼110 nm [132] to ∼120 nm [129] and to ∼125 nm [131]). In this theoretical modelling study of the distribution of alpharecoil tracks in DSDP 418A basaltic glass, we consider each alpha-recoil track to be the end result of complete U-or Thseries decay.…”
Section: Modelling Methodologymentioning
confidence: 99%
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“…As they grow-for example, during the eight successive alpha-recoil events during the complete radioactive decay chain of 238 U to 206 Pb-alpharecoil tracks typically "zigzag" through their host material (Figure 4(a)), ∼30-50 nm in new random directions with each successive alpha-recoil event (e.g., Figure 3 in Jonckheere and Gögen [131]; Table 1 in Stübner and Jonckheere [132]), resulting in a final composite cluster of radiation damage measuring about 120 nm across (e.g., estimates for the mean diameter of alpha-recoil tracks derived from the complete decay of 238 U to stable 206 Pb in micas range from ∼110 nm [132] to ∼120 nm [129] and to ∼125 nm [131]). In this theoretical modelling study of the distribution of alpharecoil tracks in DSDP 418A basaltic glass, we consider each alpha-recoil track to be the end result of complete U-or Thseries decay.…”
Section: Modelling Methodologymentioning
confidence: 99%
“…In this theoretical modelling study of the distribution of alpharecoil tracks in DSDP 418A basaltic glass, we consider each alpha-recoil track to be the end result of complete U-or Thseries decay. For example, even though a total of eight alpharecoil events take place during the complete radioactive decay of 238 U to 206 Pb, because they are all interconnected they are considered as a "single" composite ∼120 nm wide alpharecoil track (Figure 4(a) [129,131,132]). In addition, for simplicity in this high spatial resolution theoretical modelling study (Figures 10(i) and 15(c)) each alpha-recoil track is modelled as a ∼120 nm diameter sphere (instead of as myriad different geometric varieties of zigzagging structures) and this is in keeping with the observation that when fully etched, alpha-recoil tracks tend to form relatively equant etch-pits (e.g., see Figure 4(b); Figure 1 in Stübner et al [133]); that is, the theoretical nanoscopic "zigzagging" threedimensional structure of alpha-recoil tracks is effectively destroyed upon etching.…”
Section: Modelling Methodologymentioning
confidence: 99%
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“…Because the directions in which the alpha particles are emitted and the daughter nuclides recoil are random, tracks resulting from a number of successive disintegrations will be more or less equidimensional in all directions. The size distribution of recoil tracks depends on the time of track accumulation and is in general bimodal with maxima at ∼ 30 and ∼ 125 nm (Jonckheere and Gögen, 2001;Stübner and Jonckheere, 2005).…”
Section: Recoil Tracksmentioning
confidence: 99%