Abstract:Activities of 26 Al and 10 Be in five chert clasts sampled from two beach ridges of late Pleistocene Lake Lisan, precursor of the Dead Sea in southern Israel, indicate low rates of chert bedrock erosion and complex exposure, burial, and by inference, transport histories. The chert clasts were derived from the Senonian Mishash Formation, a chert-bearing chalk, which is widely exposed in the Nahal Zin drainage basin, the drainage system that supplied most of the material to the beach ridges.Simple exposure ages… Show more
“…Our dates correlate with the relative age of the terraces. Moreover, they correlate well with ages of the highest beach ridges (up to −150 m) found by Bowman and Gross (1992) in the south-west of the Dead Sea and dated by Matmon et al (2003) to 20-36 ka BP. Also our dates are consistent with the age estimates of the Lake Lisan high stand derived from dating of the Lisan Formation to 27-23 cal.…”
“…Our dates correlate with the relative age of the terraces. Moreover, they correlate well with ages of the highest beach ridges (up to −150 m) found by Bowman and Gross (1992) in the south-west of the Dead Sea and dated by Matmon et al (2003) to 20-36 ka BP. Also our dates are consistent with the age estimates of the Lake Lisan high stand derived from dating of the Lisan Formation to 27-23 cal.…”
“…Pairing cosmogenic 10 Be 181 with stable noble gases such as 21 Ne measured in quartz (Niedermann, 2000;182 Niedermann, 2002), or the longer-lived 26 Al (half-life of 0.72 Myr; Samworth et al 183 (1972) Be ratios (Granger and Muzikar, 2001; 184 Granger, 2006;Balco and Shuster, 2009), is common to e.g. extend the time frame of 185 investigation required for these applications (Granger and Muzikar, 2001;Schaller et 186 al., 2002;Matmon et al, 2003;Partridge et al, 2003;Schaller et al, 2004;Balco and 187 Stone, 2005;Stock et al, 2005;Haeuselmann et al, 2007;Kong et al, 2009;Hu et al, 188 2011;Matmon et al, 2011;Wittmann et al, 2011b;Charreau et al, 2012;Bekaddour 189 et al, 2014;McPhillips et al, 2016). Recently, the in situ-cosmogenic nuclide 14 C 190 which has a much shorter half-life of 5730 yrs (Libby, 1955) was added to the family 191 of cosmogenic isotopes measured in quartz (Lifton et al, 2001).…”
12Measured from a bag of sand taken in large rivers, the concentration of cosmogenic 13 nuclides such as in situ-produced 10 Be, 26 Al, and 14 C can be used to constrain the 14 mean sediment flux of the headwaters and assess the duration of sediment storage 15 from source to sink. We revisit these principles, with examples from the Amazon and 16
Ganga basins. 17We identify two end member cases controlling the concentration of cosmogenic 18 nuclides in lowland river sediment: 1) if the time scale of floodplain sediment storage 19 is short compared to the half-life of the nuclide, in situ cosmogenic nuclide 20 concentrations are not significantly altered in lowland basins. In this case the 21 concentration of e.g. in situ-produced 10 Be in the sediment taken in the lowland 22 2 basin equals in most cases that exported from the sediment source area, but the 23 variability in nuclide concentrations between headwater streams is significantly 24 averaged-out. Thus to convert the measured river sediments' in situ cosmogenic 25 nuclide concentration into a catchment-wide denudation rate, production rates are 26 scaled to include those of the sediment-producing mountainous areas only, rather 27 than the entire catchment area. Nuclide production in the lowlands, where no 28 sediment is being produced, is hence excluded. This correction is termed "floodplain 29 Be ratio on Be adsorbed to particles provides the denudation 51 rate. Both are similar to denudation rates from in situ 10 Be. We show that this 52 system responds more sensitively to sediment storage than the in situ system, and 53 both accumulation and decay of meteoric concentrations may thus be used to 54 determine sediment residence time. 55 56
“…Typical radiocarbon dating of shell material can suffer from potentially large reservoir corrections in alkaline lakes (Broecker and Kaufman, 1965). Conventional cosmogenic dating of shoreline berms has also proven difficult because clastic material tends to be reworked from longer-lived alluvial features, and thus suffers from inheritance of cosmogenic isotopes produced during earlier periods of exposure (Matmon et al, 2003). In contrast, shell material Wolf et al, 1998, assuming isotropic diffusion in a spherical domain driven by diffusion kinetics reported for the c-parallel direction in this paper.…”
Diffusion of helium has been characterized in four carbonates: calcite, dolomite, magnesite, and aragonite. Cleaved or oriented and polished slabs of carbonate minerals were implanted with 100 keV or 3 MeV 3 He at doses of 5 Â 10 15 3 He/cm 2 and 1 Â 10 16 3 He/cm 2 , respectively, and annealed in 1-atm furnaces. 3 He distributions following diffusion experiments were measured with nuclear reaction analysis using the reaction 3 He(d,p) 4 He.Our results show that He diffusion in calcite is the fastest among the carbonates studied, with diffusivities progressively slower in magnesite, dolomite and aragonite. In the case of the isomorphic trigonal carbonates (calcite, dolomite, magnesite), these observations are broadly consistent with predictions based on lattice characteristics such as unit cell size and inter-atomic apertures, with diffusivities faster in more open carbonate structures. Dolomite is an exception to this trend, suggesting that its unique ordered R3 crystal structure may play a role in slowing helium diffusion. Diffusion is anisotropic in all of the trigonal carbonates, and is typically slowest for diffusion along the c direction, and faster for diffusion normal to c and in directions normal to cleavage surfaces. The patterns of diffusional anisotropy are predicted to first order by the size of limiting inter-atomic apertures along any given crystallographic direction, providing additional support to the concept of modeling crystal lattices as "molecular sieves" with regard to diffusion of helium.When the effects of anisotropy and diffusion domain size are considered, our results are in reasonable agreement with previous results from bulk degassing of natural samples. Modeling of helium diffusive loss shows that calcite and magnesite are unlikely to be retentive of helium on the Earth's surface for typical grain sizes and time/temperature conditions. Dolomite and aragonite may be retentive under cooler conditions, but because helium retention is strongly dependent on diffusion domain size, general predictions are difficult given the structural complexities of natural samples. Our axis-specific diffusion measurements across a range of carbonate compositions, evaluated through direct profiling, offer important constraints for modeling helium mobility in carbonates, and for understanding the influence of the complexities of carbonate structures on He outgassing patterns.
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