1993
DOI: 10.1016/1359-0189(93)90191-b
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Track counting efficiency and unetchable track range in apatite

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Cited by 19 publications
(11 citation statements)
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“…4a curves (1) and (2)). This is in conflict with all experiments using the common etchants [12,19,24,32] and with the fact that alpha-recoil tracks are registered in the cleavage planes of muscovite [33] and [34] and but not in apatite. It is improbable that this is due to a misalignment of the apatite and muscovite during the track counts, because the 1.4 lm offset between the apatite and muscovite profiles alone requires a displacement of >13 lm in the direction of the maximum thickness gradient, which is not reconcilable with the near track-to-track match.…”
Section: Discussioncontrasting
confidence: 79%
See 1 more Smart Citation
“…4a curves (1) and (2)). This is in conflict with all experiments using the common etchants [12,19,24,32] and with the fact that alpha-recoil tracks are registered in the cleavage planes of muscovite [33] and [34] and but not in apatite. It is improbable that this is due to a misalignment of the apatite and muscovite during the track counts, because the 1.4 lm offset between the apatite and muscovite profiles alone requires a displacement of >13 lm in the direction of the maximum thickness gradient, which is not reconcilable with the near track-to-track match.…”
Section: Discussioncontrasting
confidence: 79%
“…However, the obvious cause for the difference between the measured and calculated transmission profiles is that the experiment compares the etchable track lengths with the calculated ranges of unetched latent 132 Xe and 238 U ion tracks. In materials with high registration thresholds, the distance to the point where the track-forming particle comes to rest exceeds the length over which its track is etchable; this difference is called the range deficit [17][18][19] or length deficit [12,20]. The dashed line (Fig.…”
Section: Discussionmentioning
confidence: 98%
“…In principle, a threshold of energy loss is considered to be the mechanism responsible for triggering the faster dissolution of a track core in comparison with the bulk material. However, the range deficits in apatite for external irradiations (this work; Green and Durrani 1977;Green et al 1986;Singh et al 1986;Iwano et al 1993;Alencar et al 2012) are higher than those observed for confined fission tracks Carlson et al 1999;Barbarand et al 2003b;Jonckheere 2003;Tello et al 2006), which is inconsistent with a single threshold mechanism. Recently, Li et al (2012) showed a good agreement between high-resolution measurements with electron microscopy and calculations in the electronic (inelastic) stopping power regime for the angular dispersion and width reduction of latent (non-etched) ion tracks.…”
Section: Etchlable Lengthcontrasting
confidence: 69%
“…The relatively few direct measurements of this efficiency factor range from 0.90-0.99 (e.g. Iwano et al, 1993;Jonckheere and Van den haute, 2002). Hasebe et al (2004) used a value of 1.0.…”
Section: Discussionmentioning
confidence: 99%