Florian Adolphi’s research while affiliated with University of Bremen and other places

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Publications (96)


Map of the Laptev Sea shelf showing the location of core PS2458-4 with core-top 10Be/9Be concentration (numbered coloured circle 8) and 10Be/9Be concentrations of modern surface sediments (numbered coloured circles 1–7). The dashed lines represent the reconstructed coastline extent at four different time periods (where 16 K is 16 kyrBP), with corresponding water depth values in metres shown in brackets (Klemann et al., 2015). The map was created using Ocean Data View (Schlitzer, 2016).
WAIS (orange) (Muschitiello et al., 2019; Sigl et al., 2016; Sinnl et al., 2023) and GISP2 (blue) (Finkel and Nishiizumi, 1997) 10Be fluxes corrected for correlation with ice core accumulation rates and δ18O, plotted on the IntCal20 timescale. The thick black line shows the mean of both datasets, and the bold grey line depicts the modelled oceanic 10Be signal assuming a residence time (τ) of 350 years for 10Be in the water column.
Concentrations of (a) 9Be, (b) 10Be, and (c) 10Be/9Be atomic ratios from core PS2458-4.
Sensitivity tests. (a) Three different trend fitting techniques (logarithmic, power, and LOESS). (b) Relative10Be/9Be residuals with respect to logarithmic, power, and LOESS trends.
Ice core 10Be record with τ= 350 years (blue) and the PS2458-4 record calculated from the mean of the three detrended datasets with a three-point LOESS graph using a ΔR value of 345 ± 60 14Cyears for the age model (red).

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Precise dating of deglacial Laptev Sea sediments via 14C and authigenic 10Be/9Be – assessing local 14C reservoir ages
  • Article
  • Full-text available

November 2024

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56 Reads

Arnaud Nicolas

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Johannes Lachner

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Florian Adolphi

Establishing accurate chronological frameworks is imperative for reliably identifying lead–lag dynamics within the climate system and enabling meaningful intercomparisons across diverse paleoclimate proxy records over long time periods. Robust age models provide a solid temporal foundation for establishing correlations between paleoclimate records. One of the primary challenges in constructing reliable radiocarbon-based chronologies in the marine environment is to determine the regional marine radiocarbon reservoir age correction. Calculations of the local marine reservoir effect (ΔR) can be acquired using independent 14C dating methods, such as synchronization with other well-dated archives. The cosmogenic radionuclide 10Be offers such a synchronization tool. Its atmospheric production rate is controlled by the global changes in the cosmic ray influx, caused by variations in solar activity and geomagnetic field strength. The resulting fluctuations in the meteoric deposition of 10Be are preserved in sediments and ice cores and can thus be utilized for their synchronization. In this study, for the first time, we use the authigenic 10Be/9Be record of a Laptev Sea sediment core for the period 8–14 kyr BP and synchronize it with the 10Be records from absolutely dated ice cores. Based on the resulting absolute chronology, a benthic ΔR value of +345 ± 60 14Cyears was estimated for the Laptev Sea, which corresponds to a marine reservoir age of 848 ± 90 14Cyears. The ΔR value was used to refine the age–depth model for core PS2458-4, establishing it as a potential reference chronology for the Laptev Sea. We also compare the calculated ΔR value with modern estimates from the literature and discuss its implications for the age–depth model.

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Fig 1. Map of the Arctic Ocean. The names of the marginal seas and archipelago are indicated by acronyms (BS: Beaufort Sea, CS: Chukchi Sea, LS: Laptev Sea, SV: Svalbard archipelago, FS: Fram Strait). The purple area indicates 80 the modern Yedoma domain (Strauss et al., 2021; Strauss et al., 2022; Strauss et al., 2016). The white area shows the ice sheet cover at 18 ka BP (Hughes et al., 2016; Dyke et al., 2003). Grey lines indicate the main river streams in the Arctic (Lehner and Grill, 2013). The exposed continental shelf area at 18 kyr BP is labeled in grey. The black line is the −115 m contour line, which is approximately the sea level at the early period of the last deglaciation (18 kyr BP) (Klemann et al., 2015). Yellow dots show the cores from the Arctic used in this study, including PS51/154 and PS51/159. Red dots 85 show the other cores from previous studies that are used for comparison, including cores ARA04C/37 (Wu et al., 2020), 4-PC1 (Martens et al., 2019), PC23 (Tesi et al., 2016b), PS2458 (Spielhagen et al., 2005), HH11-09 (Nogarotto et al., 2023), PS2837-5 (Birgel and Hass, 2004), and MSM05/5-712-2 (Müller and Stein, 2014; Aagaard-Sørensen et al., 2014; Zamelczyk et al., 2014). The map background is from the International Bathymetric Chart of the Arctic Ocean (IBCAO) (Jakobsson et al., 2012).
Fig 2. (a-e) The biomarker proxies from cores PS51/154 (dark blue) and PS51/159 (light green) and (f-h) environmental 270 changes in the western Laptev Sea since the last deglaciation. (a) High molecular weight (HMW) fatty acid (C26:0, C28:0, C30:0) mass accumulation rate (MAR) of cores PS51/154 and PS51/159 (this study), the MAR peaks are labeled with numbers. (b) Paq values of cores PS51/154 and PS51/159 (this study). (c) Syringic acid/syringaldehyde ratio (Sd/Sl) of cores PS51/154 and PS51/159 (this study). (d) IP25 contents of cores PS51/154 and PS51/159 (Hörner et al., 2016). (e) Age-depth model controlling points from radiocarbon dating measurements of cores PS51/154 and PS51/159. (f) Rate 275 of sea-level rise in the western Laptev Sea (Klemann et al., 2015). (g) Area of land inundation per kyr in the western Laptev Sea, calculated from the sea-level reconstruction from Klemann et al. (2015) and the bathymetric data from the international bathymetric chart of the Arctic Ocean (IBCAO) (Jakobsson et al., 2012). (h) Counts of newly developed thermokarst lakes, categorized by the basal ages of the reported thermokarst lakes (number within 500-yr bins) in Siberia (Brosius et al., 2021). The names of different paleoclimate periods are indicated by acronyms (HS1: Heinrich
Fig 5. Environmental changes since the last deglaciation and terrestrial biomarker mass accumulation rates (MARs) of core records in the Arctic Ocean and higher-latitude northern hemisphere. (a) Atmospheric CO2 concentration (Köhler et al., 2017). (b) Rate of global sea-level change (Lambeck et al., 2014). (c) Compilation of basal ages of thermokarst lakes (number within 500-yr bins) in North America (Brosius et al., 2021). (d) Campestreol+β-sitosterol MAR from core ARA04C/37, Beaufort Sea (Wu et al., 2020). (e) Lignin phenol MAR from core 4-PC1, Chukchi Sea (Martens et al., 395 2019). (f) brGDGT MAR from cores SO202-18-3/6, Bering Sea (Meyer et al., 2019). (g) Compilation of basal ages of thermokarst lakes (number within 500-yr bins) in Siberia (Brosius et al., 2021). (h) Lignin phenol MAR from core PC23, Laptev Sea (Tesi et al., 2016b). (i) HMW fatty acid MAR from core PS51/154, Laptev Sea (this study). (j) HMW fatty
Environmental controls of rapid terrestrial organic matter mobilization to the western Laptev Sea since the last deglaciation

September 2024

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294 Reads

Arctic permafrost stores vast amounts of terrestrial organic matter (terrOM). Under warming climate conditions, Arctic permafrost thaws, releasing aged carbon and potentially impacting the modern carbon cycle. We investigated the characteristics of terrestrial biomarkers, including n-alkanes, fatty acids, and lignin phenols, in marine sediment cores to understand how the sources of terrOM transported to the ocean change in response to varying environmental conditions such as sea-level rise, sea ice coverage, inland climate warming, and freshwater input. We examined two sediment records from the western Laptev Sea (PS51/154 and PS51/159) covering the past 17.8 kyr. Our analyses reveal three periods with high mass accumulation rates (MARs) of terrestrial biomarkers, from 14.1 to 13.2, 11.6 to 10.9, and 10.9 to 9.5 kyr BP. These MAR peaks revealed distinct terrOM sources, likely in response to changes in shelf topography, rates of sea-level rise, and inland warming. By comparing periods of high terrOM MAR in the Laptev Sea with published records from other Arctic marginal seas, we suggest that enhanced coastal erosion driven by rapid sea-level rise during meltwater pulse 1A (mwp-1A) triggered elevated terrOM MAR across the Arctic. Additional terrOM MAR peaks coincided with periods of enhanced inland warming, prolonged ice-free conditions, and freshwater flooding, which varied between regions. Our results highlight regional environmental controls on terrOM sources, which can either facilitate or preclude regional terrOM fluxes in addition to global controls.


Figure 1: Map of the Laptev Sea shelf showing the location of core PS2458-4 with core-top 10 Be/ 9 Be concentration 147 (numbered colored circle 8) and 10 Be/ 9 Be concentrations of modern surface sediments (numbered colored circles 1-7).
Figure 3: Concentrations of (a) 9 Be, (b) 10 Be and (c) 10 Be/ 9 Be atomic ratios from core PS2458-4
Figure 4: Sensitivity tests (a) Three different trend fitting techniques (logarithmic, power, and LOESS), (b)
Figure 5: Ice core 10 Be record with tau=350 years (blue) and PS2458-4 record calculated from the mean of the three
Figure 7. Likelihood results based on different R for the LOESS-smoothed ice core 10 Be using for different tau values 349 of 200, 350, 500 and 600 years. 350 351
Precise dating of deglacial Laptev Sea sediments via 14 C and authigenic 10 Be/ 9 Be – assessing local 14 C reservoir ages

July 2024

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121 Reads

Establishing accurate chronological frameworks is imperative for reliably identifying lead-lag dynamics within the climate system and enabling meaningful inter-comparisons across diverse paleoclimate proxy records over long time periods. Robust age models provide a solid temporal foundation for establishing correlations between paleoclimate records. One of the primary challenges in constructing reliable radiocarbon-based chronologies in the marine environment is to determine the regional marine radiocarbon reservoir age correction. Calculations of the local marine reservoir effect (ΔR) can be acquired using 14C-independent dating methods, such as synchronization with other well-dated archives. The cosmogenic radionuclide 10Be offers such a synchronization tool. Its atmospheric production rate is controlled by the global changes in the cosmic ray influx, caused by variations in solar activity and geomagnetic field strength. The resulting fluctuations in the meteoric deposition of 10Be are preserved in sediments and ice cores and can thus be utilized for their synchronization. In this study, for the first time, we use the authigenic 10Be/9Be record of a Laptev Sea sediment core for the period 8–14 kyr BP and synchronize it with the 10Be records from absolutely dated ice cores. Based on the resulting absolute chronology, a benthic ΔR value of +345 ± 60 14C years was estimated for the Laptev Sea, which corresponds to a marine reservoir age of 848 ± 90 14C years. The ΔR value was used to refine the age-depth model for core PS2458-4, establishing it as a potential reference chronology for the Laptev Sea. We also compare the calculated ΔR value with modern estimates from the literature and discuss its implications for the age-depth model.


Simulated radiocarbon cycle revisited by considering the bipolar seesaw and benthic 14C data

May 2024

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137 Reads

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1 Citation

Earth and Planetary Science Letters

Carbon cycle models used to calculate the marine reservoir age of the non-polar surface ocean (called Marine20) out of IntCal20, the compilation of atmospheric 14C, have so far neglected a key aspect of the millennial-scale variability connected with the thermal bipolar seesaw: changes in the strength of the Atlantic meridional overturning circulation (AMOC) related to Dansgaard/Oeschger and Heinrich events. Here we implement such AMOC changes in the carbon cycle box model BICYCLE-SE to investigate how model performance over the last 55 kyr is affected, in particular with respect to available 14C and CO2 data. Constraints from deep ocean 14C data suggest that the AMOC in the model during Heinrich stadial 1 needs to be highly reduced or even completely shutdown. Ocean circulation and sea ice coverage combined are the processes that almost completely explain the simulated changes in deep ocean 14C age, and these are also responsible for a glacial drawdown of ∼60 ppm of atmospheric CO2. We find that the implementation of abrupt reductions in AMOC during Greenland stadials in the model setup that was previously used for the calculation of Marine20 leads to differences of less than ±100 14C yrs. The representation of AMOC changes therefore appears to be of minor importance for deriving non-polar mean ocean radiocarbon calibration products such as Marine20, where atmospheric carbon cycle variables are forced by reconstructions. However, simulated atmospheric CO2 exhibits minima during AMOC reductions in Heinrich stadials, in disagreement with ice core data. This mismatch supports previous suggestions that millennial-scale changes in CO2 were probably not driven directly by the AMOC, but rather by biological and physical processes in the Southern Ocean and by contributions from variable land carbon storage.



Comparison between modeled ¹⁰Be outputs from GEOS‐Chem and E63H23 averaged over the period 2005–2013 and measurements from (a) Antarctica traverse, (b) Greenland traverse, and (c) a compiled deposition flux data set. Panel (d) shows GEOS‐Chem deposition fluxes averaged over 2005–2013 overplotted with measurements (color‐coded dots) from panel (c). Panel (e) shows the relative differences of modeled ¹⁰Be deposition flux (calculated as (E63H23/GEOS‐Chem‐1) × 100%) over the period 2005–2013 while the zonal mean of relative differences is shown in panel (f). For the Antarctica traverse, the model data are plotted as the latitudinal band (2‐degree) based on measurement sites. ¹⁰Be concentrations are calculated using the ¹⁰Be fluxes multiplied by the ice density and then divided by corresponding accumulation rates. For the Greenland traverse, the model lines are plotted as a function of latitudes averaged over the Greenland region. FA2 indicates the percentages of model data within the factor of 2.
(a) The sources of ¹⁰Be deposition and (b) sink fraction of ¹⁰Be production in different regions modeled from GEOS‐Chem averaged over 2005–2013. The stratospheric contributions in bracket in panel (a) are from the E63H23 simulation. Only values larger than 4% are labeled.
Simulated deposition changes for different mixing scenarios as a function of solar modulation function (Phi) and geomagnetic dipole moment. All ¹⁰Be fluxes are normalized over the Phi of 500 MeV and GMD of 7.8 × 10²² Am². The “SH” and “NH” indicate the southern hemisphere and northern hemisphere, respectively.
GEOS‐Chem modeled relative changes of ¹⁰Be deposition for the (a) solar minimum and (b) geomagnetic minimum compared to the control simulation and the corresponding zonal mean (c, d). The black dashed lines in panel (c, d) indicate the ones considering global mixing. The green crosses and orange circles indicate the relative changes inferred from measurements in ice cores and marine sediments (Adolphi et al., 2023).
Modeling Atmospheric Transport of Cosmogenic Radionuclide Be Using GEOS‐Chem 14.1.1 and ECHAM6.3‐HAM2.3: Implications for Solar and Geomagnetic Reconstructions

January 2024

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139 Reads

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4 Citations

Plain Language Summary The cosmogenic radionuclide beryllium‐10 (¹⁰Be) deposition in natural archives can be used to reconstruct solar and geomagnetic changes in the past. Understanding how ¹⁰Be deposition reflects atmospheric production rate changes is crucial for these applications. However, this relationship remains debated. To address this issue, we use two state‐of‐the‐art global models, GEOS‐Chem 14.1.1 and ECHAM6.3‐HAM2.3, along with the latest beryllium production model (CRAC: Be). When responding to solar modulation, both models indicate that ¹⁰Be deposition corresponds proportionally to global production rate changes, with a minor latitudinal bias. However, during geomagnetic modulation, ¹⁰Be deposition changes significantly compared to global production rate changes. ¹⁰Be deposition also shows varying hemispheric responses to geomagnetic modulation, attributed to the asymmetric production between hemispheres. For the extreme solar proton event in 774/5 CE, ¹⁰Be shows a higher deposition flux increase in the polar regions compared to the tropics. These findings underscore the need to account for atmospheric mixing on ¹⁰Be deposition from different locations, especially for the changes due to the geomagnetic field variations.


Simulations of 7Be and 10Be with the GEOS-Chem global model v14.0.2 using state-of-the-art production rates

December 2023

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106 Reads

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8 Citations

The cosmogenic radionuclides 7Be and 10Be are useful tracers for atmospheric transport studies. Combining 7Be and 10Be measurements with an atmospheric transport model can not only improve our understanding of the radionuclide transport and deposition processes but also provide an evaluation of the transport process in the model. To simulate these aerosol tracers, it is critical to evaluate the influence of radionuclide production uncertainties on simulations. Here we use the GEOS-Chem chemical transport model driven by the Modern-Era Retrospective analysis for Research and Applications, Version 2 (MERRA-2) reanalysis to simulate 7Be and 10Be with the state-of-the-art production rate from the CRAC:Be (Cosmic Ray Atmospheric Cascade: Beryllium) model considering realistic spatial geomagnetic cutoff rigidities (denoted as P16spa). We also perform two sensitivity simulations: one with the default production rate in GEOS-Chem based on an empirical approach (denoted as LP67) and the other with the production rate from the CRAC:Be but considering only geomagnetic cutoff rigidities for a geocentric axial dipole (denoted as P16). The model results are comprehensively evaluated with a large number of measurements including surface air concentrations and deposition fluxes. The simulation with the P16spa production can reproduce the absolute values and temporal variability of 7Be and 10Be surface concentrations and deposition fluxes on annual and sub-annual scales, as well as the vertical profiles of air concentrations. The simulation with the LP67 production tends to overestimate the absolute values of 7Be and 10Be concentrations. The P16 simulation suggests less than 10 % differences compared to P16spa but a significant positive bias (∼18 %) in the 7Be deposition fluxes over East Asia. We find that the deposition fluxes are more sensitive to the production in the troposphere and downward transport from the stratosphere. Independent of the production models, surface air concentrations and deposition fluxes from all simulations show similar seasonal variations, suggesting a dominant meteorological influence. The model can also reasonably simulate the stratosphere–troposphere exchange process of 7Be and 10Be by producing stratospheric contribution and 10Be/7Be ratio values that agree with measurements. Finally, we illustrate the importance of including the time-varying solar modulations in the production calculation, which significantly improve the agreement between model results and measurements, especially at mid-latitudes and high latitudes. Reduced uncertainties in the production rates, as demonstrated in this study, improve the utility of 7Be and 10Be as aerosol tracers for evaluating and testing transport and scavenging processes in global models. For future GEOS-Chem simulations of 7Be and 10Be, we recommend using the P16spa (versus default LP67) production rate.


Evaluating the 11-year solar cycle and short-term 10Be deposition events with novel excess water samples from the East Greenland Ice-core Project (EGRIP)

November 2023

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93 Reads

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2 Citations

10Be is produced by the interaction between galactic cosmic rays (GCRs) and solar energetic particles (SEPs) with the Earth's atmospheric constituents. The flux of GCRs is modulated by the varying strength of the magnetic fields of the Earth and the Sun. Measurement of 10Be concentrations from polar ice cores is thus a valuable tool to reconstruct the variations in the geomagnetic field and solar activity levels. The interpretation of 10Be records is, however, complicated by non-production-related effects on the 10Be deposition rate caused by climate- or weather-induced variability. Furthermore, volcanic eruptions have been proposed to lead to short-term 10Be deposition enhancements. In this study, we test the use of excess meltwater from continuous flow analysis (CFA) to measure 10Be, allowing less time-consuming and more cost-effective sample preparation. We compare two records obtained from CFA and discrete samples from the East Greenland Ice core Project (EGRIP) S6 firn core, reaching back to 1900 CE. We find that the two records agree well and that the 10Be record from CFA samples agrees as well as the discrete samples with other records from Greenland. Furthermore, by subtracting the theoretically expected GCR-induced signal, we investigate the high-frequency variability in the 10Be records from Greenland and Antarctica after 1951 CE, focusing on SEP events and volcanic eruptions. Finally, we use the 10Be records from Greenland and Antarctica to study the 11-year solar cycles, allowing us to assess the suitability of the CFA samples for the reconstruction of solar activity. This result opens new opportunities for the collection of continuous 10Be records with less time-consuming sample preparation, while saving an important portion of the ice cores for other measurements.


High-resolution aerosol data from the top 3.8 kyr of the East Greenland Ice coring Project (EGRIP) ice core

November 2023

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98 Reads

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6 Citations

Here we present the high-resolution continuous flow analysis (CFA) data from the top 479 m of the East Greenland Ice coring Project (EGRIP) ice core covering the past 3.8 kyr. The data consist of 1 mm depth-resolution profiles of calcium, sodium, ammonium, nitrate, and electrolytic conductivity as well as decadal averages of these profiles. The nominally 1 mm data represent an oversampling of the record as the true resolution is limited by the analytical setup to approximately 1 cm. Alongside the data we provide a description of the measurement setup, procedures, the relevant references for the specific methods as well as an assessment of the precision of the measurements, the sample-to-depth assignment, and the depth and temporal resolution of the data set. The error in absolute depth assignment of the data may be on the order of 2 cm; however, relative depth offsets between the records of the individual species are only on the order of 1 mm. The presented data have sub-annual resolution over the entire depth range and have already formed part of the data for an annually layer-counted timescale for the EGRIP ice core used to improve and revise the multi-core Greenland ice-core chronology (GICC05) to a new version, GICC21 . The data are available in full 1 mm resolution and decadal averages on PANGAEA (10.1594/PANGAEA.945293, ).


Solar, Atmospheric, and Volcanic Impacts on Be Depositions in Greenland and Antarctica During the Last 100 Years

August 2023

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184 Reads

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6 Citations

Cosmogenic radionuclides (e.g., ¹⁰Be) from ice cores are a powerful tool for solar reconstructions back in time. However, superimposed on the solar signal, other factors like weather/climate and volcanic influences on ¹⁰Be can complicate the interpretation of ¹⁰Be data. A comprehensive study of ¹⁰Be records over the recent period, when atmospheric ¹⁰Be production and meteorological conditions are relatively well‐known, can improve our interpretation of ¹⁰Be records. Here we conduct a systematic study of the production and climate/volcanic signals in Antarctica and Greenland ¹⁰Be records, including a new ¹⁰Be record from the East GReenland Ice‐core Project site. Greenland and Antarctica records show significant decreasing trends (5%–6.5%/decade) for 1900–1950, which is comparable with the expected production rate inferred from sunspot observations. By comparing ¹⁰Be records with reanalysis data and atmospheric circulation patterns, ¹⁰Be records from Southern/Southeastern Greenland are significantly correlated with the Scandinavia pattern. Stacking ¹⁰Be records from different locations can enhance the production signal. However, this approach is not always straightforward as uncertainties in some records can lead to a weaker solar signal. A strategy can be employed to select records for the bipolar stack by comparing Greenland records with Antarctica records, assuming the shared signal is a production signal. Finally, we observe significant increases (36%–64%) in ¹⁰Be depositions in Greenland related to the Agung eruption. This large increase in Greenland ¹⁰Be records after the Agung eruption, could be partly explained by the enhanced air mass transport from mid‐latitudes coinciding with the decreased precipitation en‐route.


Citations (70)


... Complemented by an expanded global network of 14 C measurements, such an approach would allow the use of observed latitudinal gradients in the amplitude of ESPEs 50 . Similar chemical transport models could be used to simulate the dispersal and fallout of 10 Be and 36 Cl on polar ice caps 95,102 . This is crucial because aerosols from volcanic eruptions can increase the deposition of 10 Be and 36 Cl, generating abrupt spikes that may be confused with ESPEs 103 . ...

Reference:

Extreme solar storms and the quest for exact dating with radiocarbon
Modeling Atmospheric Transport of Cosmogenic Radionuclide Be Using GEOS‐Chem 14.1.1 and ECHAM6.3‐HAM2.3: Implications for Solar and Geomagnetic Reconstructions

... For transport/convection, GEOS-Chem was run at 600 s temporal resolution, and for chemistry/emission, at a 1200 s resolution. Instead of using the default beryllium production rate by [7], we ran GEOS-Chem with updated production rates for beryllium provided by [39]. These updated production rates are 3-dimensional and temporally varying, and are based on the latest production model called CRAC:BE (Cosmic Ray-Induced Atmospheric Cascade for Beryllium) [14]. ...

Simulations of 7Be and 10Be with the GEOS-Chem global model v14.0.2 using state-of-the-art production rates

... However, the Sun often also exhibits violent behavior, which sporadically results in flares or coronal mass ejections (CMEs) that liberate into interplanetary space intense fluxes of SEPs, orders of magnitude more energetic than ordinary solar cosmic rays (Kovaltsov et al. 2012;Usoskin 2017). When such SEPs hit Earth, they could trigger exceptional production of cosmogenic nuclides, even though the direct observational evidence of this phenomenon is limited (Paleari et al. 2023;Pedro et al. 2012;Usoskin et al. 2020). For instance, the strongest solar storm that happened to hit the Earth in recent history, the Carrington Event of 1859 CE, left no trace in available cosmogenic nuclide records (McCracken et al. 2001;Scifo et al. 2019;Smart et al. 2006;Wolff et al. 2012). ...

Evaluating the 11-year solar cycle and short-term 10Be deposition events with novel excess water samples from the East Greenland Ice-core Project (EGRIP)

... In Table 2, we list the averages of L1 and L2 for a rise of 10 %-90 % and decay of 90 %-10 %, respectively. L1 and/or L2 are often defined as the depth resolution of a CFA system Erhardt et al., 2023;Grie-man et al., 2022). This definition gives a depth resolution of 35-40 mm for the δ 18 O, Na, and rBC data over the depth interval between 6.17 and 112.87 m. ...

High-resolution aerosol data from the top 3.8 kyr of the East Greenland Ice coring Project (EGRIP) ice core

... For 10 Be, local climate factors can be important, meaning that multiple ice cores from different geographic locations must be used (e.g. Muscheler et al., 2007;Zheng et al., 2023;Golubenko et al., 2022). Accounting for these factors allows the radionuclide production rate to be estimated, from which we can infer the GCR flux at the top of the atmosphere. ...

Solar, Atmospheric, and Volcanic Impacts on Be Depositions in Greenland and Antarctica During the Last 100 Years

... Details of conventional and AMS radiocarbon ages in Late Holocene soils of the Rouge Catchment, South Central Ontario Notes: Finite ages (R13, R13A horizons 1 and 3, R47-Ahb, R47B and WD5) were calculated using Oxcal and the IntCal20 calibration curve(Reimer et al. 2020;Bronk Ramsey et al. 2023); post-bomb values were calculated using Calib.org/CALIBomb(Reimer and Reimer 2024 CALIBomb [WWW program] at http://calib.org ...

DEVELOPMENT OF THE INTCAL DATABASE

Radiocarbon

... In order to overcome these issues, we need to add to the radiocarbon clock, which has always ticked with two hands, a third one and to do so, we need to combine different scientific disciplines and different points of view, what we call: "the multidisciplinary approach" (Talamo et al., 2023a). Here I will present the upgrade of radiocarbon to substantially increase the resolution of the radiocarbon calibration curve after 15,000 years ago, as well as the tight error range that characterizes the 14C age (Talamo et al., 2023a(Talamo et al., , 2023b. In addition, we will show how to determine the presence of collagen on bone samples using advanced spectrometric methods, such as near-infrared hyperspectral imaging (NIR-HSI), which results in diminishing the destruction of valuable material (Malegori et al., 2023). ...

Atmospheric radiocarbon levels were highly variable during the last deglaciation

... Cheng et al., 2018Cheng et al., , 2021 provides further motivation for re-assessing the synchronization between the Greenland ice-core and U-Th timescales. Lastly, there is a need for improved constraints during the Last Glacial Maximum (LGM), i.e., when the timescales reach their largest offset according to cosmogenic radionuclides Sinnl et al., 2023), and assess possible fast changes in the timescale difference that are currently challenging to detect. ...

Synchronizing ice-core and U / Th timescales in the Last Glacial Maximum using Hulu Cave 14C and new 10Be measurements from Greenland and Antarctica

... The EGRIP CFA data were measured by the Bernese setup and the data set is available at PANGAEA with the measurements described by Erhardt et al. (2023). In addition to the CFA system already successfully deployed for the NEEM ice core, the setup was extended by an inductively coupled plasma time-of-flight mass spectrometer (icpTOF, TOFWERK, Thun, Switzerland). ...

High resolution aerosol data from the top 3.8 ka of the EGRIP ice core

... McCracken (2004) proposed another purely empirical approach linking the 10 Be production to its deposition by using various ad-hoc assumptions of atmospheric mixing and their latitude dependence. We note that such simplistic approaches are still in use (e.g., Adolphi et al., 2023) because of the lack of a readily applicable full model. Field et al. (2006) developed the first beryllium transport model based on the Goddard Institute for Space Studies general circulation model (GISS GCM ModelE). ...

On the Polar Bias in Ice Core Be Data