L.K. Fifield’s research while affiliated with Australian National University and other places

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Publications (393)


Topographic map of the Republic of South Africa and the state territory of Lesotho. Sampling locations are highlighted by tear pins. Administratively, the investigated sites are located within the Free State Province of the Republic of South Africa. The province largely stretches across the Highveld ecoregion, which resembles an elevated, open-grassland plain landscape.
Changes in topsoil fallout inventories (a) and bulk soil organic carbon (SOC) content (b; Lobe et al., 2001) over time, as well as the correlation of the SOC and 239+240Pu concentrations (c). The inventories in cultivated soils are shown relative to those found in adjacent native grassland soils (i.e. 100 % at t=0). The mono-exponential regression (thin black line, enveloped by grey 68 % confidence interval) in (a) indicates the approach towards a concentration equilibrium level after about 20–40 years of cropping. By that time, about 50 %–60 % of the initial 239+240Pu inventory has been lost. The extrapolated post-35-year cropping equilibrium level is indicated by the dashed line. The relationship between 239+240Pu and SOC indicates that the decrease in SOC can be traced by measuring 239+240Pu in bulk soil (c). Most plutonium samples depict replicate measurements; the corresponding activities are weighted means and the uncertainties dominated either by AMS counting statistics (weighted mean error) or by external sources of uncertainty (standard error). For single measurements, the 1σ measurement uncertainty provided by the AMS facilities dominates the final uncertainty. All greyed-out data points with dashed error bars denote those samples that were taken from plots with more than 32 years of cultivation history (for discussion see text). Filled circles denote samples from the Harrismith (HS) agroecosystem, filled triangles those from the Kroonstad (KR) agroecosystem, and filled diamonds those from the Tweespruit (TW) agroecosystem. Numbers in brackets denote correlation coefficients (R2).
Correlation of 137Cs and 239+240Pu topsoil activities. 137Cs data are shown with 1σ uncertainties (which equal the estimated measurement errors). 239+240Pu activities were mostly measured in replicate, and the corresponding concentrations are weighted means and the uncertainties dominated either by AMS counting statistics (weighted mean error) or by external sources of uncertainty (standard error). For single measurements, the 1σ measurement uncertainty provided by the AMS facilities dominates the final uncertainty. The majority of samples overlap with the linear regression (black line) and its 68 % confidence interval (in grey). Sample HS0/0-20 has been excluded from the regression (greyed out; for discussion see text). The extrapolated regression intersects the ordinate at about 0.0050 mBqg-1 (0.50 mBqkg-1; unit conversion to mBqg-1 due to lower-level precision achieved by γ spectrometry). 137Cs data have been decay-corrected to February 2012 (the time of measurement).
The 239+240Pu inventories at depth (20–40 cm) compared to corresponding topsoil activities (0–20 cm). The analysis of plutonium activities at depth has been conducted for n=6 samples, belonging to the agroecosystems Tweespruit (0, 32, 40, and 60 years of cultivation) and Harrismith (0 and 45 years of cultivation). At all sites but HS45, the nuclide concentration is significantly lower at depth than close to the surface. Error bars are 1σ uncertainties (see Fig. 2 for details).
Plutonium concentrations link soil organic matter decline to wind erosion in ploughed soils of South Africa
  • Article
  • Full-text available

February 2025

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123 Reads

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Hendrik Wiesel

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Loss of soil organic matter (SOM) from arable land poses a serious threat to soil fertility and crop yields, and it thwarts efforts to conserve soils as carbon sinks to mitigate global warming. Wind erosion can be a major factor in the redistribution of soil fines including SOM, but assessments of its impact have typically been limited by short observation periods of a few years at most. Longer time frames, extending back to the mid-20th century, may however be probed using the concentrations of radionuclides that were globally distributed by nuclear weapon tests conducted during the 1950s and early 1960s. The basic concept is that differences in fallout radionuclide (FRN) activities between undisturbed and arable soils can be used to infer soil particle redistribution. In the present work, we have measured activities of 137Cs and 239+240Pu in soils from three agricultural regions of the plains of the South African Highveld. The three regions represent distinct agroecosystems, and within each region the temporal length of cultivation varies from 0 (i.e. native grassland) to almost 100 years. Wind erosion has previously been shown to play a dominant role in soil particle loss from agricultural sites in the Highveld, and the level plots we investigate here did not show any evidence of fluvial erosion. Hence, we interpret the fate of soil fines, including SOM, to be governed by wind erosion. For the cultivated soils, radionuclide activities are found to be less than in adjacent native grassland, and the magnitude of the reduction is strongly correlated with the duration of cultivation. Specifically, the original inventories of both 137Cs and 239+240Pu are approximately halved after ∼20–40 years of cropping. The initial rate loss relative to the undisturbed soils is, however, considerably higher, with ∼6%yr-1 recorded during the first year after native grassland is converted to arable land. We correlate our radionuclide data with previously published SOM contents from the same sampled material and find that the radionuclides are an excellent indicator of SOM decline at the sites we investigate. We conclude that wind erosion can exert a dominant control on SOM loss in arable land of South Africa.

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Toward defining the Anthropocene onset using a rapid increase in anthropogenic fingerprints in global geological archives

September 2024

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235 Reads

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5 Citations

Proceedings of the National Academy of Sciences

One of the remaining issues regarding the Anthropocene is the lack of stratigraphic evidence indicating when the cumulative human pressure from the early Holocene began to fundamentally change the Earth system. Herein, we compile anthropogenic fingerprints from various high-precision-dated proxy records for 137 global sites to determine the age of the unprecedented surge in these records over the last 7700 y. The cumulative number of fingerprints revealed an unprecedented surge in diverse anthropogenic fingerprints starting in 1952 ± 3 CE, corresponding to the onset of the Great Acceleration. Notably, the period from 1953 to 1958 CE saw a nearly simultaneous surge in fingerprints across all regions, including Antarctica, the Arctic, East Asia, Europe, North America, and Oceania. This synchronous upsurge reflects the moment when human impacts led to rapid transformations in various natural processes and cycles, with humans becoming a geological force capable of inscribing abundant and diverse anthropogenic fingerprints in global strata. Following this global fingerprint explosion, profound planetary-scale changes, including deviations from the established natural climatic conditions, begin. This unprecedented surge in anthropogenic signals worldwide suggests that human influences started to match many natural forces controlling the processes and cycles and overwhelm some of the functioning of the Earth system around 1952.


Figure 1: Topographic map of the Republic of South Africa and the state territory of the Kingdom of Lesotho. Sampling locations are highlighted by tear pins. Administratively, the investigated sites are located within the Free State Province of the Republic of 670 South Africa. The province largely stretches the Highveld ecoregion, which resembles an elevated, open grassland plain landscape.
Figure 2: Changes in topsoil fallout concentrations (A) and soil organic carbon (SOC) content (B; Lobe et al., 2001) in the soil 680 fraction <20 µm over time, and correlation of the two variables (C). The concentrations in cultivated soils are shown relative to those found in adjacent native grassland soils (i.e., 100% at t = 0). The mono-exponential regression (thin black line, enveloped by grey 68% confidence interval) in panel (A) indicates the approach towards a concentration equilibrium level after about 25-45 years of cropping. By that time, about 50-60% of the initial 239+240 Pu concentration has been lost. The extrapolated post-32 years cropping equilibrium level is indicated by the dashed line. The relationship between 239+240 Pu and SOC in the clay and silt fractions indicate 685 that the decrease of SOC can be traced by measuring 239+240 Pu in soil fines (C). Most plutonium samples depict replicate measurements; the corresponding concentrations are weighted means and the uncertainties either dominated by AMS counting statistics (weighted mean error) or external sources of uncertainty (standard error). For single measurements, the 1σ measurement uncertainty provided by the AMS facilities dominates the final uncertainty. All greyed out data points with dashed error bars denote those samples that were taken from plots with more than 32 years of cultivation history (for discussion see text). Filled circles denote 690 samples from the Harrismith (HS) agroecosystem; filled triangle those from the Kroonstad (KR) agroecosystem and filled diamonds those from the Tweespruit (TW) agroecosystem.
Figure 4: Correlation of 137 Cs and 239+240 Pu topsoil activities. 137 Cs data are shown with 1σ uncertainties (which equal the estimated measurement errors). 239+240 Pu activities were mostly measured in replicate, and the corresponding concentrations are weighted 715 means and the uncertainties either dominated by AMS counting statistics (weighted mean error) or external sources of uncertainty (standard error). For single measurements, the 1σ measurement uncertainty provided by the AMS facilities dominates the final uncertainty. The majority of samples overlap with the linear regression (black line) and its 68% confidence interval (in grey). Sample HS0/0-20 has been excluded from the regression (greyed out; for discussion see text). The extrapolated regression intersects the ordinate at about 0.0050 mBq g -1 (0.50 mBq kg -1 ; unit conversion to mBq g -1 due to lower level precision achieved by γ spectrometry). 720 137 Cs data have been decay-corrected to February 2012 (the time of measurement).
Figure 5: 239+240 Pu concentrations at depth (20-40 cm) as compared to corresponding topsoil activities (0-20 cm). The analysis of plutonium activities at depth has been conducted for n = 6 samples, belonging to the agroecosystems Tweespruit (0, 32, 40, and 60 years of cultivation) and Harrismith (0 and 45 years of cultivation). At all sites but HS45, the nuclide concentration is significantly lower at depth than close to the surface. Error bars are 1σ uncertainties (see Fig. 2 for details).
Agroecosystem details.
Plutonium concentrations link soil organic matter decline to wind erosion in ploughed soils of South Africa

June 2024

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112 Reads

Losses of soil organic matter (SOM) from arable land poses a serious threat to soil fertility and crop yields, and thwarts efforts to conserve soils as carbon sinks to mitigate global warming. Wind erosion can be a major factor in the redistribution of soil fines including SOM, but assessments of its impact have typically been limited by short observation periods of a few years at most. Longer timeframes, extending back to the mid 20th century, may however be probed using the concentrations of radionuclides that were globally distributed by nuclear weapon tests conducted 1950s and early 1960s. The basic concept is that differences in fallout radionuclide (FRN) activities between undisturbed and arable soils can be used to infer soil particle redistribution. In the present work, we have measured activities of 137Cs and 239+240Pu in soils from three agricultural regions of the plains of the South African Highveld. The three regions represent distinct agroecosystems and within each region the temporal length of cultivation varies from zero (i.e., native grassland) to almost 100 years. The sampled plots did not show any evidence of fluvial erosion, allowing the contribution of wind erosion to the loss of soil fines, including SOM, to be investigated. For the cultivated soils, radionuclide activities are found to be less than in adjacent native grassland, and the magnitude of the reduction is strongly correlated with the duration of cultivation. Specifically, the original concentrations of both 137Cs and 239+240Pu are approximately halved after ~25–45 years of cropping. The initial rate loss relative to the undisturbed soils is, however, considerably higher, with ~6 % yr-1 recorded during the first year after native grassland is converted to arable land. We correlate our radionuclide data with previously published SOM contents from the same sampled material and find that the radionuclides are an excellent indicator of SOM decline at the sites we investigate. We conclude that wind erosion can exert a dominant control on SOM loss in arable land of South Africa and by implication at comparable settings on Earth.


Locations of the soil cores and groundwater monitoring. FFRC: Fukushima Forestry Research Center. Core samples were collected in Koriyama (A), (B), Yamakiya. The variation in groundwater table was measured at site (C), as shown in Supplementary Fig. S4. The edited map is cited from the original map of (https://www.gsi.go.jp/tizu-kutyu.html). The map of the copyright holder is the Geospatial Information Authority of Japan.
Correlation between the one-dimensional migration analyses in the unsaturated soil layer (0–6 m) and the vertical distribution of the ³H and ³⁶Cl radionuclide released during the Fukushima nuclear accident, March 11th, 2011. (a) The distribution of the measured ³H (atoms L⁻¹) concentration in the unsaturated soil (0.05–4.25 m) and saturated soil zones (4.25–6 m) on Sep. 24th, 2014, 3.6 years after the accident. (b) The distribution of the measured ³⁶Cl concentration (atoms L⁻¹) in the unsaturated soil (0.05–4.25 m) and saturated soil zones (4.25–6 m) on Sep. 24th, 2014. (c) Distributions of the hydro tracers (³H and ³⁶Cl) transported by the rainwater that precipitated on March 15th, 2011, were estimated by one-dimensional analytical solutions via the dispersion (D = 0.039 m² year⁻¹) and vertical infiltration rate of soil water (v = 0.95 m year⁻¹) in the unsaturated soil layer at Koriyama in Fukushima. Black solid (³H) and dash (³⁶Cl) lines: 1 year later, blue line: 2 years later, red line: 3.6 years later. Decay of ³H has been included.
Distributions of the hydro tracers (³H and ³⁶Cl) transported by the rainwater that precipitated on March 15th, 2011, were estimated by one-dimensional analytical solutions. (a) Koriyama in Fukushima Prefecture. Black solid (³H) and dash (³⁶Cl) lines: 1 year later, blue line: 2 years later, red line: 3.6 years later, yellow dashed line: 5.7 years later. One-dimensional analytical solutions were estimated via the dispersion (D = 0.039 m² year⁻¹) and vertical infiltration rate of soil water (v = 0.95 m year⁻¹) in the unsaturated soil layer. (b) Yamakiya in Fukushima Prefecture. Black solid (³H) and dash (³⁶Cl) lines: 1 year later, blue line: 2 years later, red line: 3.6 years later, yellow dashed line: 5.7 years later. One-dimensional analytical solutions were estimated via the dispersion (D = 0.060 m² year⁻¹) and vertical infiltration rate of soil water (v = 2 m year⁻¹) in the unsaturated soil layer. Yamakiya belongs to granite area which has flow-path fractures and the vertical infiltration rate would be ≥ 2 m year⁻¹. The water table is below 10 m.
The distributions of the ³H (TU) and ³⁶Cl (atoms L⁻¹) concentrations in unsaturated soil water (collected in 2014 at Koriyama and in 2016 at Koriyama and Yamakiya) and shallow groundwater (collected at Koriyama in 2020 and 2021 at a depth of 6.8 m and 6.5 m below the surface) relative to the zone of natural ³H (< 6 TU) and ³⁶Cl (< 4.6 × 10⁶ atoms L⁻¹) deposition measured in 2014 and 2016 in Fukushima. The light gray area indicates the possible range of natural fallout of ³H and ³⁶Cl. The black dashed line shows the maximum ³⁶Cl concentration deduced from the maximum deposition flux in the spring peak observed at Tsukuba¹² and annual precipitation of Koriyama. The blue dashed line shows the average natural concentration of ³⁶Cl estimated from the average annual deposition flux observed at Tsukuba¹² and annual precipitation of Koriyama.
Record of H and Cl from the Fukushima nuclear accident recovered from soil water in the unsaturated zone at Koriyama

November 2023

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62 Reads

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2 Citations

The opportunity to measure the concentrations of ³H and ³⁶Cl released by the Fukushima nuclear accident in 2011 directly in rain was lost in the early stage of the accident. We have, however, been able to reconstruct the deposition record of atmospheric ³H and ³⁶Cl following the accident using a bore hole that was drilled in 2014 at Koriyama at a distance of 60 km from the accident. The contributions of ³H and ³⁶Cl from the accident are 1.4 × 10¹³ and 2.0 × 10¹² atoms m⁻² respectively at this site. Very high concentrations of both ³H (46 Bq L⁻¹) and ³⁶Cl (3.36 × 10¹¹ atoms L⁻¹) were found in the unsaturated soil at depths between 300 and 350 cm. From these, conservative estimates for the ³H and ³⁶Cl concentrations in the precipitation in the ~ 6 weeks following the accident were 607 Bq L⁻¹ and 4.74 × 10¹⁰ atoms L⁻¹, respectively. A second hole drilled in 2016 showed that ³H concentrations in the unsaturated soil and shallow groundwater had returned to close to natural levels, although the ³⁶Cl concentrations were still significantly elevated above natural levels.





Accelerator mass spectrometry with ANU’s 14 million volt accelerator

January 2023

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54 Reads

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11 Citations

Nuclear Instruments and Methods in Physics Research Section B Beam Interactions with Materials and Atoms

Accelerator Mass Spectrometry (AMS) at the Department of Nuclear Physics and Accelerator Applications (Australian National University) is based on a 14UD tandem accelerator. The 14UD has demonstrated exceptional accelerator performance over more than three decades of AMS, e.g. by running regularly above 14 MV. We present the actual performance for the whole range of measured radionuclides and the potential of this specialised high-energy AMS facility - demonstrating the continuing need for such a system. Focus here will be also on the unique setup comprising an Enge split-pole spectrograph used as a gas-filled magnet (GFM). The GFM has seen growing importance at ANU over the years as a means for providing an efficient reduction of isobaric background. We use the Enge now routinely for ¹⁰Be, ²⁶Al, ³²Si, ⁵³Mn and ⁶⁰Fe measurements.


The impact of the break-up of molecules in the stripper on the AMS performance

December 2022

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28 Reads

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3 Citations

Nuclear Instruments and Methods in Physics Research Section B Beam Interactions with Materials and Atoms

The break-up of molecules in the stripper of an AMS facility induces an energy and angular spread in the beam. This can cause beam losses, thereby reducing the performance of an AMS facility. With an appropriate design, these effects can be minimised and the efficiency enhanced. As an example, the break-up of BeO molecules is discussed here. First the basic physics is described and corresponding models and computer codes are explained. Then experimental data are shown and compared with the models. For gas stripping, beam profiles are available for small and large facilities. All show tails which can be attributed to the dissociation of the molecules. The size of the effect depends on various parameters such as beam energy, selected charge state, stripping gas type and ion optics. Foil stripping leads to energy distributions which are much wider, and show typically a double peak.


Element separation chemistry and cosmogenic 10Be dating of a ferromanganese crust

November 2022

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79 Reads

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10 Citations

Nuclear Instruments and Methods in Physics Research Section B Beam Interactions with Materials and Atoms

Oceanic archives are contemporary witnesses of Earth’s recent astrophysical history by incorporating extraterrestrial radionuclides. VA13/2 - 237KD is one of the most studied ferromanganese crusts and it has been shown that the crust contains live interstellar ⁶⁰Fe. Here, we have characterized a large piece of this crust with a 3D optical scan, a micro-CT scan and 3D modeling, followed by the chemical extraction of highly purified, element-specific fractions for accelerator mass spectrometry. High-accuracy cosmogenic ¹⁰Be dating of two independent drill-holes showed a time-dependent variability in growth rate across the surface of the crust. This well-characterized crust is used to search for interstellar radionuclides, such as supernova-produced ⁶⁰Fe and the r-process nuclide ²⁴⁴Pu. Other extraterrestrial radionuclides including ²⁶Al, ⁵³Mn, ¹²⁹I, ¹⁸²Hf or ²⁴⁷Cm could be investigated in the future.


Citations (76)


... These authors, who elsewhere advocate using 'events' to describe vague and diachronous phenomena are in this instance actually using the term appropriately, and as applied by the AWG. Geologically abrupt events are in practice commonly used to guide the position of GSSPs for chronostratigraphic units, and Waters et al. (2022; see also Kuwae et al., 2024) noted the numerous distinct events that cluster around the mid-20th century where they provide ample means of and justification for identifying a GSSP for the Anthropocene. ...

Reference:

Response to Damianos—Anthropocene angst: Authentic geology and stratigraphic sincerity
Toward defining the Anthropocene onset using a rapid increase in anthropogenic fingerprints in global geological archives

Proceedings of the National Academy of Sciences

... The velocity of the atomic ions impinging onto the stripper medium is responsible for the charge state yield, which depends on the molecular mass before breakup and the terminal voltage. Significant transmission losses can occur due to Coulomb explosion for molecular ions when employing a foil stripper which are reduced but still present for gas stripping (Fifield et al. 2023). ...

Coulomb explosion of BeO− molecular ions – Revisited
  • Citing Article
  • May 2023

Nuclear Instruments and Methods in Physics Research Section B Beam Interactions with Materials and Atoms

... Samples were measured via ICP-AES (Thermo Fisher Scientific Inc., ICP-OES-iCAP7400) using an internal yttrium standard. 9 Be concentrations were calculated using standard addition following Ellison & Thompson [12] and Kelly et al. [17]. Apart from Be we also measured Al, B, Ca, Co, Fe, K, Mn, Ni, P, Si, Ti, V and Zn via ICP-AES but without standard addition. ...

Cosmogenic 10Be and 26Al sample preparation at the University of Wollongong
  • Citing Article
  • February 2023

Nuclear Instruments and Methods in Physics Research Section B Beam Interactions with Materials and Atoms

... Its presence was shown through an elevated 60 Fe/Fe ratio by single-atom counting (i.e. accelerator mass spectrometry (AMS), [3][4][5]) in several deep-ocean samples a e-mails: d.koll@hzdr.de; dominik.koll@anu.edu.au ...

Accelerator mass spectrometry with ANU’s 14 million volt accelerator
  • Citing Article
  • January 2023

Nuclear Instruments and Methods in Physics Research Section B Beam Interactions with Materials and Atoms

... Our transmission levels are lower than what could be expected from the previous reports of Be yields in O 2 or Ar gas [3,4]. This could be due to losses in the stripper canal or due to an incomplete measurement of the Be 2+ intensity caused by the energy spread of the beam after the Coulomb explosion in the stripper [28,29]. ...

The impact of the break-up of molecules in the stripper on the AMS performance
  • Citing Article
  • December 2022

Nuclear Instruments and Methods in Physics Research Section B Beam Interactions with Materials and Atoms

... Both radionuclides are measured at the Heavy-Ion Accelerator Facility (HIAF) of the Australian National University (ANU) [4], which is currently the only facility capable of measuring these radionuclides with the required sensitivity after the closure of the Munich accelerator lab [10]. The measurements of 244 Pu require uttermost sensitivity and, therefore, the dedicated setup of VEGA at the Australian Nuclear Science and Technology Organisation (ANSTO) [27] with the highest sensitivity for actinide measurements [28] is currently used. In the future, actinide measurements are expected to be continued at the newly installed Helmholtz Accelerator Mass Spectrometer Tracing Environmental Radionuclides (HAMSTER) facility at Helmholtz-Zentrum Dresden-Rossendorf (HZDR), where the measurement of further radionuclides such as 182 Hf might also become feasible. ...

Element separation chemistry and cosmogenic 10Be dating of a ferromanganese crust
  • Citing Article
  • November 2022

Nuclear Instruments and Methods in Physics Research Section B Beam Interactions with Materials and Atoms

... At the LE side, a NEC MC-SNICS 32-sample ion source is installed ( Figure F.10). The sputter voltage is typically 3 -5 kV and was recently reduced to 2 kV exclusively for volatile beams such as Cl − and I − (Fifield et al. 2022). The negative ion beam is extracted by 150 kV and analysed by the 90 • injection magnet with a bending power of mE q 2 = 56 MeV amu. ...

Backgrounds and blanks in Iodine-129 measurements at the Australian National University
  • Citing Article
  • November 2022

Nuclear Instruments and Methods in Physics Research Section B Beam Interactions with Materials and Atoms

... They also demonstrated the capability to quantify 210 Pb in small-mass materials such as Kapton films, reaching specific activity limits below 3 Bq·kg −1 in sub-gram samples. The Australian National University developed techniques for ultra-trace 210 Pb detection in NaI crystals used in dark matter experiments, achieving 210 Pb/Pb ratios as low as 10 −16 by employing high-purity carrier materials [12]. Our work continues this progression by addressing a critical gap: the effective extraction and purification of trace 210 Pb from metallic copper, a material widely used in low-background detector construction. ...

Scavenger hunt: Searching for the optimal target material for low-level 210Pb accelerator mass spectrometry
  • Citing Article
  • October 2022

Nuclear Instruments and Methods in Physics Research Section B Beam Interactions with Materials and Atoms

... The Silurian-Devonian strata form the hilly areas in the south and around the study area, and the Cretaceous strata form the lowland areas (Figures 1 and 2). Blockfields due to Pleistocene periglacial climate are found in Australia; however, they are as far south as 30 S (Slee et al., 2022), which is 1600 km away from Black Mountain at 15 40 0 S ( Figure 1). ...

The age and paleoclimate implications of relict periglacial block deposits on the New England Tablelands, Australia

Quaternary Research

... Nevertheless, for this mass range, it is quite challenging to deal with the interference caused stable isobars: 91 Zr in the case of 91 Nb; 94 Zr and 94 Mo in the case of 94 Nb; and 93 Nb in the case of 93 Mo. For these relative differences in the atomic number of ΔZ/Z close to 1/100, isobar separation techniques based on the difference in energy loss reach their limit, even with terminal voltages above 8.5 MV and foil stripping [20,21,22,23,24]. This paper presents the preliminary studies on the capability of the Ion-Laser InterAction Mass Spectrometry (ILIAMS) setup of the 3-MV-AMS facility VERA (Vienna Environmental Research Accelerator) at the University of Vienna [25,26,27] ...

Accelerator mass spectrometry measurements of 93Zr for astrophysical and nuclear technology applications
  • Citing Article
  • September 2022

Nuclear Instruments and Methods in Physics Research Section B Beam Interactions with Materials and Atoms