Abstract
Cosmogenic radionuclide 10Be and 26Al targets (BeO and Al2O3) for AMS analysis are produced by a growing number of geochemical laboratories, employing different sample processing methods for the extraction of Be and Al from environmental materials. The reliability of this geochronological tool depends on data reproducibility independent from the preparation steps and the AMS measurements. Our results demonstrate that 10Be and 26Al concentrations of targets processed following different, commonly used protocols and measured at two AMS facilities lead to consistent results. However, insoluble fluoride precipitates, if formed during processing, can cause decreased 26Al results, while 10Be concentrations are unaffected.
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Introduction
Cosmogenic in situ produced radionuclides (CRN) are widely used in geomorphology and Quaternary geology by allowing direct age determination of landforms and measurement of denudation rates over 102 to 106 timescales [1,2,3]. However, the power of this geochronological tool strongly depends on the accuracy, precision and reproducibility and thus comparability of data provided by different laboratories, both for sample preparation and for Accelerator Mass Spectrometry (AMS) measurements. It is critical for the reliability of the results to obtain the same nuclide concentrations within uncertainties for a sample, regardless of the methodology followed during sample processing and AMS measurement.
In this study, an inter-laboratory comparison of two different sample processing methodologies carried out at two cosmogenic nuclide sample preparation laboratories (Cosmo-lab) is presented. The main objective of the comparison was to verify if CRN results are independent of the sample processing method and of the involved laboratory facility. At BudapestFootnote 1 chemical sample processing followed the procedures used at LN2C (CEREGE, Aix en Provence) adapted from Brown et al. [4], Merchel and Herpers [5] and also described by Merchel et al. [6] (MH). At Vienna,Footnote 2 procedures adapted from Kohl and Nishiizumi [7] and Granger et al. [8] were followed (KNG).
Although the quartz purification and geochemical procedures for rock digestion and ion separation are well-described for both protocols, several potential complications exist. In particular, insoluble metal-fluoride precipitation during sample dissolution and evaporation and its effect on trapping 10Be and 26Al was monitored. For this purpose, the full MH nuclide extraction protocol was compared to a simplified and faster version of the same protocol to test if results are robust using the fast track. Also, the suitability of the Microwave Plasma – Atom Emission Spectrometry (MP-AES) method for the determination of the total Al content of the samples was tested. One further goal was to monitor the background in the Cosmo-labs of Budapest and Vienna to see if it was low enough for reliable and repeatable cosmogenic nuclide data production.
These objectives are achieved by the comparison of the 10Be and 26Al concentrations in quartz in aliquots of a natural sample set of 12 samples from a fluvial terrace of the Danube River and in six aliquots of the CoQtz-N reference quartz material [9] processed using both MH and KNG extraction schemes. From the CoQtz-N two additional aliquots were processed by the KNG scheme only for 10Be determination.
For two samples (Dan14-14 and -25) no comparison is possible because only a single assay was processed. Their 10Be and 26Al concentrations are included in this study in order to provide the complete dataset for further use.
Theory
Cosmogenic in situ produced 10Be and 26Al are formed by the interaction of secondary cosmic rays with Si and O in quartz and are retained in the mineral lattice [10]. They are radioactive with half-lives of 1.387 ± 0.012 Ma for 10Be [11, 12] and 0.705 ± 0.017 Ma for 26Al [13]. Their concentration in quartz at the time of sampling depends on their production by cosmic rays and loss by radioactive decay and denudation. Pure quartz mineral separates are required for extraction of cosmogenic 10Be and 26Al to resolve geological and geomorphological issues as their productions have been calibrated within this mineral [1,2,3]. However, the direct comparison and joint analysis of the published results relies on the hypothesis that the reported cosmogenic 10Be and 26Al concentrations are similar within uncertainties, regardless of the facility and protocol of sample preparation and AMS device involved in the data acquisition. The present study aims at testing this hypothesis.
Experimental
Sample collection
The Vienna Basin is located between the Eastern Alps and the Western Carpathians and developed during the Miocene [14]. Fluvial terraces located on intra-basinal hills [15, 16] within the extensional structure of the Vienna Basin have been dissected by faults related to the Vienna Basin Transform Fault.
The sample set was taken from a 12 m thick fluvial sandy-gravel succession of a terrace on the intra-basinal hills south of the Danube east of the village of Haslau an der Donau (48.1141 N, 16.74342E, 189 m asl.; 40 m relative height Figs. 1, 2). Based on geomorphological mapping, its age is Middle Pleistocene [17], and thus within the range of burial age determination using the cosmogenic nuclide pair of 10Be and 26Al. The samples were taken from the undisturbed terrace material exposed in an active gravel pit (Figs. 1, 2).
Samples for CRN analysis were collected from 5.5 m and 11.5 m subsurface depths. At each level six quartz cobbles were taken from the cobble-rich sandy gravel (Fig. 2). The cobbles were either quartzite or hydrothermal bluish (vein) quartz. At the base of the quarry, muscovite-rich upper Miocene (Pannonian) sand was exposed.
Physical sample processing
The goal of physical sample processing is to remove accessory minerals and thus to obtain a quartz-enriched sample aliquot. The cobbles were washed to remove attached grains, crushed and sieved and the 250–1000 µm grain size fraction of each sample was split into two sub-samples that were processed at the two laboratories. The crushed cobbles were magnetically separated in Vienna. In Budapest density separation using LST fastfloat was applied to remove heavy minerals and feldspars, if necessary.
Chemical sample processing
The first phase of chemical sample processing is chemical etching of the samples. The objective in this phase is to dispose of minerals that are not completely removed by physical treatment. For instance, intergrown minerals of the feldspar group are often still present in the physically cleaned quartz. A second objective of the chemical etching of the quartz is to remove atmospheric 10Be that may be adsorbed to the surface of quartz grains or in fissures within the mineral. Tables 1 and 2 present the successive steps applied at each lab needed to reach pure mineral separate.
The purity of the sample can be tested by different methods. For instance, microscopy [6] in combination with XRD to determine its mineralogy or by digesting a small aliquot to determine its Al content using ICP. If the quartz is successfully purified and is low in Al, it can pass to the next sample preparation phase, when cosmogenic 10Be and 26Al are released from the quartz lattice by total dissolution of the sample.
Once pure quartz is obtained and carefully weighted, 9Be carrier is added before its total dissolution. 9Be is always added because the natural 9Be is too low to ensure an accurate determination of the 10Be/9Be ratio. The amount of 9Be in the sample is calculated from the carrier weight, no additional measurement is involved. 27Al carrier may be added together with the 9Be or just before ion chromatography, depending on the timing of the determination of the natural Al content of the samples. 27Al carrier is added only if the natural Al content is too low; however, in most cases its addition is not required.
The purified quartz is dissolved in HF by the formation of SiF4. As HF solution is not easy to handle, it is evaporated leaving behind elements from within the quartz lattice in a precipitate (“cake”). This precipitate can vary considerably in size depending on the purity of the quartz (i.e. the mass of elements trapped in the lattice, and also on the success of quartz purification during the previous sample preparation steps) and may contain metal-fluorides. To break-up these insoluble metal-fluorides they are converted into soluble chlorides by HClO4 (MH scheme) or sulfates by H2SO4 (KNG scheme).
In the next phase all interstitial ions that were trapped in the quartz crystal itself are removed and Be and Al are extracted and purified by using a combination of ion exchange chromatography and pH selective precipitation.
During the last steps of sample processing hydroxides are converted into metal oxides (BeO and Al2O3) and targets for AMS measurement are prepared to determine their 10Be/9Be and 27Al/26Al ratios.
The samples were processed following the MH and KNG procedures (Tables 1 and 2, respectively). In addition, the reduced MH protocol, without the fluoride conversion step using HClO4 (step 2.3.2. in Table 1) was tested on all samples (MH1 and MH2 sample batches, Tables S 2 and S4,). This simplification is resulting in a faster, more simple evaporation procedure. However, when omitting the step of breaking up the insoluble metal fluorides, the samples are more prone to the formation of a fluoride precipitate during evaporation.
In case a substantial, light-greyish-yellow precipitate formed during the evaporation of the HF-HNO3 solution to dryness (Dan14-12, -13, -14; -21 and -22 in MH1 and MH2 batches of simplified protocol), the addition of nitric acid and further heating was not sufficient to re-dissolve this precipitate. Therefore, the clear supernatant solution was transferred into centrifuge tubes and the precipitate was rinsed twice with 7.1 M HCl and once with H2O and left in the PTFE beakers. To ensure that no precipitate was transferred, the solute was centrifuged, rinsed again, 2 times with 7.1 M HCl, once with H2O and the clear supernatant was transferred into a new tube. This clear solution was further processed (Figs. 3, 4).
The main goal of this test was threefold: (1) to test the performance of the faster protocol (2) to investigate the effect of the insoluble precipitates on the calculated 26Al and 10Be concentrations of the samples; (3) to reveal if Be or Al are trapped linearly, or Be is not sensitive to precipitate formation, as it was suggested for fluoride precipitates formed during feldspar digestion and evaporation [18].
All the samples where fluoride precipitate was formed using the simplified protocol were re-processed using the full protocol (except for Dan14-14, see the Aluminium-26 results section, Table 3). 10Be and 26Al concentrations of both sub-samples were determined in order to quantify the effect of Al and Be trapping in the insoluble fluorides. A control sample (Dan14-23) with no precipitate formation in the simplified protocol was also re-processed. Then the resulting 10Be and 26Al concentrations were compared to each other and to the assays processed using the full KNG protocol.
It has to be emphasized that the quality of the purified quartz is of major importance for several reasons:
-
i)
as it has been mentioned above, the production of 10Be and 26Al have been calibrated within quartz only and therefore the presence of other minerals with different production rates of 10Be and 26Al (as they may have different amount of target elements such as O, Si, Al) will lead to a bias during the determination of the production time span;
-
ii)
presence of Al-bearing minerals and impurities within the quartz during the evaporation step after HF digestion may produce huge precipitates that retain Al, and make it impossible to determine the correct amount of 27Al necessary to calculate the 26Al amount after AMS measurement. Fortunately, according to a previous study where precipitates formed during feldspar digestion were tested, Be is not most probably not affected by the presence of these precipitates [18].
-
iii)
in samples with high 27Al content it may be problematic to obtain a perfect separation of Be and Al during the ion exchange chromatography. The presence of Al in BeO will alter the emission current when performing the AMS measurement and may thus results in a lower counting statistics. In such cases the use of multiple cationic exchange resin steps and/or larger ion exchange columns may help reducing the 27Al content in the BeO target [19?].
It has to be noted that the CoQtz-N reference material was purified quartz [9], therefore it was used without any quartz purification steps (processed from steps 2.1 onwards in Tables 1, 2).
The main differences between the chemical sample processing are
-
i)
The method of quartz cleaning,
-
ii)
The timing of carrier addition and determination of Al content in an aliquot,
-
iii)
The sample dissolution temperature,
-
iv)
The agent used to convert metal-fluorides into soluble form,
-
v)
The ion exchange column types and volumes,
-
vi)
The timing of pH selective precipitation.
Determination of the 27 Al concentration
It is essential to know the exact amount of Al in the dissolved sample for the calculation of its 26Al concentration. For this purpose, an aliquot must be taken from the solution and its Al concentration was determined using Inductively Coupled Plasma Mass Spectrometry (Agilent ICP-MS 7500 at the Geological Survey of Austria, Vienna), Inductively Coupled Plasma-Optical Emission Spectrometry (ICP-OES; ICAP 6500 from Thermo at CEREGE, Aix en Provence, France; and a Perkin Elmer Optima 8300 ICP-OES at BOKU, Vienna, Austria) and Microwave Plasma – Atom Emission Spectrometry (Agilent 4100 MP-AES at the Institute of Nuclear Research, Debrecen, Hungary). As MP-AES is not as widely used for the determination of the stable (natural, native) Al content of samples, therefore for some samples the native Al content was determined using both the ICP-OES and MP-AES methods, in order to test the accuracy and precision of this method.
Accelerator mass spectrometry measurements
AMS measurements were performed at ASTER, the French national facility, CEREGE, Aix en Provence [19] and at VERA, Vienna Environmental Research Accelerator, Faculty of Physics, University of Vienna.
At ASTER BeO was mixed with Niobium powder in Cu cathodes. Samples were normalized to the standard STD11 with an assigned 10Be/9Be ratio of (1.191 ± 0.013) × 10–11 [20]. Aster terminal voltage is set at 4.5MV, BeO− is stripped to Be2+ within the terminal (stripper gas is Argon at 1.2 × 10–2 mBar) then to Be4+ after the absorber foil (SiN) used to separate Be from B [19]. At VERA, samples were normalized to the standard SMD-Be-12 [21]. Both standards are comparable with KNSTD [22] with a 10Be half-life of 1.387 Myr. The uncertainty of the reference material is included in the reported uncertainties. At VERA 10Be was measured using isobar suppression with a foil stack absorber [23] technique. At the maximum terminal voltage of 3 MV and an argon stripper areal density of ~ 4 µg/cm2 this detection method allows the high energy beam of 10Be2+ to impact on the absorber foils and the directly following gas-filled ionization chamber. Depending on the 10B and 9BeH content of each sample the detector electronics may have to process additional events, produced by ions which were not stopped or even created in nuclear reactions in the SiN foils. These events can be separated from the 10Be by their energy loss in the detector volume but need to be considered for a correct live time estimation of the measurement. In this study, this showed to be a particular requirement and was guaranteed by an electronic pulser module producing ~ 70 artificial counts per second.
26Al samples measured at ASTER (extracted as Al− and measured under the Al3+ form) were normalized to the standard SM-Al-11 with a 26Al/27Al ratio of (7.401 ± 0.064) × 10–12 with a terminal voltage set at 2.7 MV [19], and those measured at VERA were normalized to SMD-Al-11. Both are secondary standard materials directly traceable to primary standards [19, 24, 25]. At VERA 26Al is measured with the ILIAMS method [26] where an AlO− beam is injected into a radiofrequency quadrupole and overlapped with a laser beam. With this technique, the interfering isobar MgO− can be suppressed by 14 orders of magnitude, resulting in machine blank levels of 5∙10–16. The 26Al ions are counted in a gas-filled ionization chamber in the charge state 3 + to avoid interferences from 13C1+. The maximum yield for the 3 + state was found for argon stripping at 2.9 MV with a stripper gas density of ~ 3 µg/cm2. Since the stripper gas pressure measurement at the terminal is technically challenging and the density profile in the tube is generally unknown, the areal density for the stripper gas at VERA can only be estimated.
At ASTER, both Be and Al samples are measured three times for 20 min divided in 40 blocks of 30 s each. At the end of the batch, for a given sample, these three measurements are compared and recombined to provide the 10Be/9Be or 26Al/27Al measured ratios. Uncertainties are taking into account the counting statistics of each sample, the standard variability within the entire batch, the standard uncertainties and for 10Be a 0.5% external uncertainty [19].
Results
Beryllium-10 results
Beryllium results are presented in Supplementary Tables S1 and S2. With the MH protocol, the measured 10Be/9Be ratio of the samples varied between (1.54 ± 0.06)E-13 and (2.76 ± 0.19)E-14 for the natural (Haslau) samples and between (8.59 ± 0.19)E-13 to (7.22 ± 0.27)E-13 for the reference material (CoQtz-N) assays. With the KNG protocol, the 10Be/9Be ratio of the Haslau samples was between (2.84 ± 0.06)E-13 and (4.17 ± 0.18)E-14 and between (6.59 ± 0.32)E-13 and (8.59 ± 0.19)E-13 for the CoQtz-N samples. The mean 10Be/9Be ratio of the process blanks was (5.06 ± 0.90)E-15 and (3.33 ± 0.66)E-15 with the MH and KNG protocols, respectively. The analytical uncertainties of the 10Be/9Be ratios of the samples had a mean of 5.1 and 5.7% for the MH and KNG protocols. The reported uncertainties include the 9Be carrier concentration, weighing and the AMS measurements (including the process blanks) and standards’ uncertainties.
The 10Be concentrations of the CoQtzMH assays and of 4 out of 5 CoQtzKNG assays were identical within 1σ uncertainties with the reference value [9] (Fig. 5A). The 10Be concentration measured for the CoQtzKNG-17 assay is 11% lower than the reference value, being just out of the 1σ confidence interval. All 10Be concentrations of duplicate samples from the Haslau quarry processed using the MH protocol are in good agreement with each other and overlap with the results of the assays processed using the KNG scheme within 2σ. (Table S1; Fig. 6).
Aluminium-26 results
Aluminium concentrations are listed in Supplementary Tables S3 and S4. For assays of the Haslau samples processed using the MH scheme, the measured 26Al/27Al ratio varied between (2.98 ± 1.66)E-13 and (1.71 ± 0.0.30)E-14 and from (2.81 ± 0.07)E-12 to (2.49 ± 0.14)E-12 for the CoQztMH assays. The Haslau samples processed using the KNG protocol had a ratio from (4.74 ± 0.20)E-13 to (2.73 ± 0.28)E-14, and the CoQtzKNG samples were between (1.89 ± 0.09)E-12 and (2.13 ± 0.07)E-12. The reported uncertainties of the 26Al concentrations include 27Al carrier concentration as given on certificate, weighing, measurement of the total Al content and the analytical uncertainties of AMS measurements and standards including the process blanks. The mean 26Al/27Al ratio of the blanks of the MH protocol was (7.05 ± 2.41)E-15. For batches MH1, MH3 and MH4 the 26Al/27Al ratio of the process blanks was below the detection limit and the sample ratios were corrected with the machine blanks. The mean blank ratio for the KNG samples was (8.27 ± 6.39)E-16. The Blk ratio of the KNG2 batch was zero, therefore this sample was not blank corrected. The mean analytical uncertainty of the samples was 11% for the MH samples (excluding the unusually high 56% value of the Dan14-10 sample due to low current at AMS) and 9% for the KNG scheme.
The 26Al concentrations of two out of the three CoQtzMH samples were at the reference value [9], while one sample (CoQtz-N-Bp19/1) was slightly higher, but still in agreement within 1σ uncertainty (Fig. 5B, Table S4). The 26Al concentrations calculated using the native Al concentrations determined either by ICP-OES or MP-AES agreed within error (as described in the Discussion) and the weighted mean of the two 26Al values was used for the comparison to the reference value. The 26Al concentration of the CoQtzKNG17 sample was matching the reference value, and the CoQtzKNG15 and -16 values were slightly higher (21% and 18%, respectively) just outside the 1σ uncertainty range (Fig. 5B).
At first glance the 26Al concentrations of the samples show a puzzling picture where different assays of some samples are matching (Dan14-10, -11, -15, -23), while others are considerably lower than their duplicate(s) (Dan14-12, -13, 21, -22) (Table S4, Fig. 7). The samples with the low concentrations that do not match their pairs are coincident with the assays that were affected by the formation of a visible precipitate after evaporation using the simplified MH procedure.
The precipitates were examined using X-Ray Diffraction (XRD) at the Geological and Geochemical Research Institute in Budapest (Rigaku Miniflex 600 X-Ray Diffractometer, Cu Kα radiation, 40 kV, 20 mA) and in most cases proved to be Aluminium-fluorides and in some cases, also contained insoluble minerals of metamorphic origin like pyrophyllite (Dan14-12), zircon (Dan14-12, -13) or kyanite (Dan14-14).
The alumosilicate kyanite was also independently detected in the Vienna sub-sample of Dan14-14 by XRD at the Clay Mineralogical Laboratory of the Institute of Applied Geology (Panalytical X’Pert PRO diffractometer, Cu Kα radiation, 40 kV, 40 mA). This sample was then skipped as the hot H2SO4 digestion most likely dissolved kyanite and in this way added unaccounted Al to the sample.
Discussion
Well-matching Beryllium-10 records—no risk of Beryllium loss due to fluoride precipitate
The different protocols regarding total digestion, purification, and chromatography resulted in consistent 10Be concentrations for the Haslau samples and for the CoQtz-N reference material. The latter originates from a surface sample [9], thus it has considerably higher CRN concentration per g quartz compared to the Haslau samples. The well-matching 10Be concentrations of the sample duplicates processed via the simplified and the full protocol imply a correct 10Be determination. The reported full-process blank 10Be/9Be ratios ensure that the background at both facilities involved in the study is low enough to deliver reliable and repeatable data. All 10Be concentrations overlap within error (Fig. 6). Accordingly, our results are in accordance with [18] suggesting that 10Be concentrations are unaffected by the fluoride precipitates and robust even in case some precipitate was formed during its evaporation to dryness.
Fluoride precipitate as a potential trap of Aluminium
The 26Al/27Al ratios of the full-process blanks were low enough to guarantee that the background at both facilities was low enough to deliver reliable and repeatable data. During evaporation of the HF-HNO3 solution (step 2.3 in Tables 1, 2) insoluble fluoride precipitate was formed in several samples when using the simplified MH protocol. All samples affected by visible fluoride precipitate, were also processed using the full MH protocol, except for the problematic Dan14-14 (Tables 3 and S4). The full protocol involves addition of 5 ml HClO4 (70%) to break up metal-fluorides converting them into soluble metal-chlorides (Table 1). Using the full-protocol all samples were devoid of fluoride precipitation, except for Dan14-12. Due to the persistent presence of fluoride precipitates, this sample was not further processed using the MH scheme.
26Al concentrations of the full protocol sub-samples were considerably higher compared to those processed via the simplified protocol. The assays unaffected by fluoride precipitates had similar concentrations, regardless of the protocol used for their processing (Table S4 and Fig. 7). This suggests that if the fluoride precipitate was not formed or it was successfully broken up by HClO4 addition, all Al was available in soluble chloride form and no loss of Al occurred. Accordingly, the in the absence of fluoride precipitates after evaporation duplicate samples provide comparable and repeatable results.
The only outlier is sample KNG3-Dan14-13 (Fig. 7). Al concentrations in sample splits processed using the simplified and full MH protocols follow the expected trend: the 133 ± 49 kat/gSiO2 increased to 409 ± 48 kat/gSiO2 when no fluoride precipitates were formed. Surprisingly, the 26Al concentration of the KNG assay resulted in 147 ± 10 kat/gSiO2 (mean of two measured targets), and is thus similar to the MH sub-sample affected by Al loss even though no precipitation was observed. The KNG3-Dan14-13 sample also had a higher 10Be value (Fig. 6), therefore this assay is most likely an analytical outlier for both Al and Be concentrations for the KNG scheme.
Generally, fluoride precipitates are more prone to form in samples with high natural Al content (Table S4). Excess Al might be present in a sample if the purified quartz contains traces of Al-bearing minerals (e.g. feldspars, mica). In some cases, it might be present in the quartz lattice itself [27]. Accordingly, the thorough cleaning of quartz must be the first step in preventing fluoride precipitation, followed by breaking up any fluorides that might happen to form during sample dissolution and evaporation [6].
Comparison of ICP-OES and MP-AES for the determination of the 27 Al concentration
In five samples (three CoQtzMH assays and samples: MH3-Dan14-20 and -23, the native Al concentration was determined by both ICP-OES and MP-AES (Tables S3 and S4). The Al concentrations determined by ICP and the MP were consistent within 1–7%. This translates to a final difference of 1–4% for the 26Al results. (Fig. 8A, B).
Obviously, the measured Al content has a larger effect on samples with high natural Al content. Samples with low native Al content (like the CoQtz-N samples) are less affected by the result of the measured native Al concentration, as the carrier added contributes the major part of the total Al content of these samples. In addition, aliquots with high Al concentration must be more diluted before ICP or MP measurements, which is also a potential source of error. These facts call attention to the importance of reduction of natural Al in the quartz separate as much as possible by thorough purification of quartz.
Conclusions
Two different sample processing protocols KNG and MH (Kohl and Nishiizumi [7] updated by Granger et al. [8] and Merchel and Herpers [5]) regarding total digestion, purification, and chromatography followed by two independent cosmogenic nuclide sample preparation facilities resulted in consistent 10Be and 26Al concentrations.
Formation of insoluble fluoride precipitate during sample digestion and evaporation may lead to considerable loss of Al and lowered 26Al concentrations. Therefore, the addition of a strong oxidizing agent, such as HClO4 or H2SO4 at the end of sample evaporation to break up fluorides is strongly recommended. The use of 26Al concentrations of samples that were affected by fluoride precipitation is not possible for geochronological purposes. Samples with high natural Al content are more prone to fluoride precipitation, therefore we emphasize the need for a thorough quartz purification before the extraction of in-situ produced cosmogenic Al from the crystal lattice to minimise the natural Al content of the samples.
Our experiment demonstrated that 10Be concentrations are unaffected by the fluoride precipitates and thus 10Be concentrations can be used with confidence even for these problematic samples.
Additionally, the parallel measurement of natural Al concentrations by MP-AES and ICP-OES provided similar results suggesting that both methods are suitable for the determination of the total Al content of the samples.
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Acknowledgements
The presented research was supported by the projects NKFIH 124807; OMAA 90öu17, 98öu17 and Erasmus plus. The measurements performed at the ASTER AMS national facility (CEREGE, Aix en Provence) were supported by the INSU/CNRS, the French Ministry of Research and Higher Education, IRD and CEA. Measurements of CoQtzMH assays performed at VERA were supported by the Radiate Transnational Access 19001688-ST. We are indebted to Attila Demény for his support of the launching and setup of the Cosmo-lab in Budapest. We are grateful to Silke Merchel, Greg Chmiel and Tom Clifton for their useful advice on chemistry and laboratory setup, to Marcel Hirsch for the ICP-OES measurements at BOKU, to Máté Szabó for the XRD measurements, and for István Hegyi for his help in solving any unexpected laboratory issues. Stefanie Maierhofer helped with the section in Fig 1. Three anonymous Reviewers are acknowledged for their constructive comments.
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Ruszkiczay-Rüdiger, Z., Neuhuber, S., Braucher, R. et al. Comparison and performance of two cosmogenic nuclide sample preparation procedures of in situ produced 10Be and 26Al. J Radioanal Nucl Chem 329, 1523–1536 (2021). https://doi.org/10.1007/s10967-021-07916-4
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DOI: https://doi.org/10.1007/s10967-021-07916-4