A database of radiogenic Sr–Nd isotopes at the “three poles”
- 1State Key Laboratory of Cryospheric Science, Northwest Institute of Eco-Environment and Resources, Chinese Academy of Sciences, Lanzhou 730000, China
- 2State Key Laboratory of Earth Surface Processes and Resource Ecology, Beijing Normal University, Beijing 100875, China
- 3College of Urban and Environmental Sciences, Northwest University, Xi'an 710127, China
- 4Centre for Ice and Climate, Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
- 5School of Spatial Informatics and Geomatics Engineering, Anhui University of Science and Technology, Huainan 232001, China
Correspondence: Cunde Xiao (email@example.com)
The radiogenic isotope compositions of strontium (Sr) and neodymium (Nd) on the surface of the Earth are powerful tools for tracing dust sources and sinks on the Earth's surface. To differentiate between the spatial variabilities in eolian dust sources in key cryospheric regions at the three poles (the Arctic; Antarctica; and the “third pole”, covering the high mountainous area in Asia), a dataset of Sr–Nd isotopic compositions from extremely cold or arid terrestrial environments was compiled, similar to the method of Blanchet (2019). The database includes Holocene and Quaternary snow, ice, sand, soil (loess), sediment, and rock samples from the three poles based on 90 different references and our own measurement data, with a total of 1989 data points, comprising 206 data points with different grain sizes and 212 data points with fraction measurements. There are 485 data points from the third pole, 727 data points from the Arctic, and 777 data points from Antarctica. The sampling and measurement methods of these data are introduced. For each pole, geographical coordinates and other information are provided. The main scientific purpose of this dataset is to provide a Sr–Nd dataset based on collective documentation and our own measurements, which will be useful for determining the sources and transport pathways of dust in snow, ice, rivers, and oceans at or near the three poles as well as to investigate whether multiple dust sources are present at each of the poles. This dataset provides exhaustive detailed documentation of the isotopic signatures at the three poles during specific time intervals in the Quaternary period, which are useful for understanding the sources or sinks of eolian dust and sediments at the three poles. The dataset is available from the National Tibetan Plateau Data Center (https://doi.org/10.11888/Cryos.tpdc.272100, Du, 2022).
The role of mineral dust in the Earth system extends well beyond its impact on the energy balance and involves interactions with the carbon cycle and glacier melting on global scales (Skiles et al., 2018; Shao et al., 2011). The transport of dust from the low midlatitudes, which contain major deserts that are dust sources, to the Arctic region or Antarctic ice sheet (AIS) is sensitive to amplified high-latitude climatic variability (Bory et al., 2003a, b; Lupker et al., 2010; Lambert et al., 2013; Struve et al., 2020). The isotopic compositions of the radiogenic elements strontium (Sr) and neodymium (Nd) are powerful tools for tracing dust sources and sinks because their characteristics vary significantly on the surface of the Earth (including snow, sand, sediment, loess, and eolian deposits) (Grousset et al., 1992; Chen et al., 2007; Xu et al., 2012; Robinson et al., 2021). Therefore, the combination of different isotopic signatures, specifically and (expressed as εNd(0)), has proven to be useful in discriminating among different dust source areas in Earth science.
The transport of eolian dust from natural desert regions has also been identified in modern snow and ice records at the so-called “third pole” based on Sr–Nd data (Wu et al., 2010; Xu et al., 2012; Du et al., 2015; Dong et al., 2018). Many studies have focused on dust transport from the western Chinese deserts to the Chinese Loess Plateau (CLP), Pacific Ocean, and even the Greenland ice sheet (GrIS) (Biscaye et al., 1997; Chen et al., 2007; Wei et al., 2021). However, it is still a controversial issue; for example, recent results have emphasized that eolian dust from local sources contributes significantly to high-mountain glaciers (Du et al., 2019a; Wei et al., 2021). Additionally, eolian dust from various source regions, including the Saharan Desert in North Africa and the Gobi and Taklimakan deserts in Asia, can be transported to the GrIS, and great uncertainties still exist (Han et al., 2018).
The Sr–Nd data from snow layers in the Berkner Island ice sheet in western Antarctica, for most of the year, support scenarios that involve contributions from proximal sources (Bory et al., 2010). The Sr–Nd data from insoluble dust in snow samples from East Antarctica indicate that long-distance natural dust primarily originates from Australia and that local dust originates from ice-free areas (Du et al., 2018). The Sr–Nd data from the Taylor Glacier zero-age ice samples and snow samples from Roosevelt Island could be explained by a mixture of at least two local sources (Winton et al., 2016; Aarons et al., 2017). The Sr–Nd data from Holocene ice cores from East Antarctica indicate a well-mixed atmospheric background involving a mixture of two or more sources in the Southern Hemisphere (SH) (Aarons et al., 2016, 2017; Delmonte et al., 2019). The amount of isotopic information is currently adequate for Patagonian and non-Patagonian mineral dust exported from southern South America (SSA) and the East Antarctic ice sheet (EAIS) (Grousset et al., 1992; Gaiero et al., 2007; Delmonte et al., 2010a, b, 2019; Delmonte et al., 2013; Blakowski et al., 2016; Aarons et al., 2017). Major efforts have attempted to solve the “puzzle” of the origin of the potential source areas that contribute dust to the Southern Ocean (SO) and the whole AIS (Gili et al., 2022). However, Sr–Nd data are unevenly distributed across the entire AIS. Measuring the Sr–Nd isotopic compositions in ice cores from Antarctica is a major challenge.
Although considerable Sr–Nd data have been measured, the variations in the characteristics and measurement methods of these data make it necessary to reassess these data on the dust sources in these remote regions. Therefore, the Sr–Nd data obtained from snow, soil, sediment, sand, and other samples should be integrated into a dataset to better serve the environmental and climatic sciences studying the three polar regions in the future. The answers to various questions have been hindered by a paucity of Sr–Nd data, which provide information on potential local and distal dust sources. For these reasons, we measured Sr–Nd data in some samples and collected Sr–Nd data from the literature for the three poles (Fig. 1, Table 1). The objective of this work was to produce a compilation of published and unpublished data from the three poles, and the specific time intervals of Sr–Nd data were limited to the Quaternary period. Furthermore, modern dust (Holocene) in snow or ice and sediment samples from the three poles is further discussed, and the potential dust transport paths in the GrIS and AIS are traced. Similar to the method of Blanchet (2019), here, we compile published and unpublished Sr–Nd data with an integrated filtering system from three remote poles, in which these data were collected in extremely cold and arid environments, and most of the data have not been included in previously published datasets. The dataset will help trace modern natural dust, reconstruct past environments, and extend the database of terrestrial and marine radiogenic Sr and Nd isotope data in the Earth and environmental sciences.
2.1 Sample collection and measurement
Sr–Nd data from snow, sand, soil, cryoconite, loess, and sediment samples from the three poles (namely the high mountainous regions in Asia, the Arctic, and Antarctica) were collected from our own research and existing literature (Fig. 1). Sr–Nd data from the third pole cover the area from 40 to 23∘ N and from 106 to 61∘ E and include data from arid deserts and mountains in northern China (Fig. 2). Sr–Nd data from the Arctic include data from the high Arctic to sub-Arctic areas, and Sr–Nd data from Antarctica refer to data from the area including the entire Antarctic continent, the AIS, and the Antarctic Peninsula (>60∘ S). Sr–Nd data were also collected from Australia, SSA, southern Africa (SA), and New Zealand (Fig. 1). Cryoconite refers to mixtures and/or aggregates of biotic and abiotic impurities on glacial ice, and the cryoconite samples were collected from positions at different elevations on glaciers (Table 2). Note that the ages of the snow, ice core, surface eolian dust, and deposit samples are almost all less than 1 Myr. Therefore, the ages of the Sr–Nd data in this dataset are limited to the Quaternary period.
In this study, 2 sand samples from Kangerlussuaq in West Greenland, 4 sand samples from on King George Island, and 11 sand samples from Inexpressible Island in the Ross Sea in West Antarctica were collected and measured. In general, the upper 2 or 5 cm of surface topsoil (sand) was collected with a trowel and stored in precleaned plastic bags or bottles. The sediment samples from shelves and ridges in the Arctic Ocean (AO), which were mostly retrieved from core archives, were collected through subsampling the upper surface of the core tops (with rare exceptions) (Maccali et al., 2018). Different grain sizes (<5, <10, 30, <63, <75, <100 µm, and bulk fractions) of surface soil or sand were extracted by the sieving method (Chen et al., 2007; Maccali et al., 2018; Du et al., 2018, 2019a, b; Wei et al., 2021).
Snow samples were collected from a snow pit at a vertical resolution of 5–20 cm, following the clean-hands protocol, with sampling personnel wearing integral Tyvek® bodysuits, non-powdered gloves, and masks to avoid possible contamination (Xu et al., 2012). In this study, one 1.0 m snow pit with a resolution of 10 cm was dug in the GrIS, and four fresh snow samples (M1, M2, M3, and M4) were sampled on sea ice in the AO during the Multidisciplinary Drifting Observatory for the Study of Arctic Climate (MOSAIC) mission in October 2020. Surface (2–10 cm) fresh-snow samples at different resolutions (with different thicknesses, widths, and lengths) from the Greenland and Antarctica ice sheets were excavated and placed in 5 L Whirl-Pak bags (Du et al., 2018, 2019a, b). Three horizontal snow layers were collected in Greenland and Antarctica snow pits (Bory et al., 2003b, 2010). The dust in the ice cores was extracted using the same method as that for the snow samples. Snow or ice core samples represent either bulk samples or have different grain sizes (>0.2, >0.45, >0.45, and <30 µm) (Du et al., 2015, 2019b; Bory et al., 2003a, b, 2010; Lupker et al., 2010; Wu et al., 2010).
2.2 Data processing
Sr–Nd isotope datasets from snow, ice cores, sand, sediment, soil, and loess samples from the third pole, the Arctic, and Antarctica were compiled. Data were collected from 90 different references with 2847 data points. In total, 485 data points were collected from the third pole, 727 data points were collected from the Arctic, and 777 data points were collected from Antarctica. In addition, 259 data points were collected from the pan-third pole (including the Tibetan Plateau, the Pamirs, Hindu Kush, Tienshan, the Iranian Plateau, Caucasus, the Carpathians, and the surrounding deserts), and 181 data points were included from potential source areas (PSAs) in the SH. Details on the geographical coordinates and original information can be found in this dataset, and the locations of these samples are shown on maps (Figs. 2, 4, 5, and 7). To keep the naming scheme uniform, the dataset assembled the names of each sample based on the work by Blanchet (2019). This dataset was built by incorporating data from the literature and our own database; in particular, units, source or sink, and geographical coordinates are marked in the dataset. Note that whether the Sr–Nd data represent source or sink information needs to be further determined by the detailed depositional environment or sampling locations. For example, the loess samples from the CLP represent a sink, but they also represent a dust source for the Pacific Ocean. Therefore, these samples were marked as a mixture. The sediment samples from the coasts of the SO or AO (rivers and dune sand) were also marked as a mixture. An overview of the input data is shown in Table 1. This study focuses on large amounts of different data, including data on snow, ice, sand, soil, loess, and sediment. These data are based on our own measurements, author contributions (data published), and literature searches.
All procedures were performed in clean lab facilities. The sand, loess, sediment, cryoconite, and dust samples extracted from snow and ice cores were generally digested with ultrapure acid (HNO3, HF, and HClO4, or HNO3, HF, and HCl), and and ratios were determined using different types of thermal ionization mass spectrometry or multiple-collector inductively coupled plasma mass spectrometry. Sr–Nd values, with uncertainties expressed as (2 standard errors of the mean), can also be found in the original references. The isotopic composition is expressed as follows:
where ()CHUR=0.512638. Here, CHUR stands for the chondritic uniform reservoir and represents a present-day average Earth value ()CHUR=0.512638 (Jacobsen and Wasserburg 1980).
3.1 Reliability assessment for the differences in Sr–Nd based on grain sizes as well as on lithogenic and measuring methods
The grain-size effect in different samples resulted in variations in the ratios and εNd(0) values. In the surface eolian sand and marine sediment samples, the variations in size-separated values are affected by grain size (Chen et al., 2007; Tütken et al., 2002). The Sr isotope ratios in loess from the CLP tended to be higher in the fine fraction and were much higher in the <2 µm fraction than in the coarser fractions (Rao et al., 2006). However, the variations in the isotopic ratios in alpine soils on the Tibetan Plateau (TP) are not clearly related to the grain-size effect (Lin and Feng, 2015). The εNd(0) values clearly exhibit less grain-size-dependent variability, as εNd(0) values seem not to be fractionated among mineralogically different grain-size fractions during the sedimentary cycle (Tütken et al., 2002). A substantial proportion of Sr–Nd isotope values showed enrichment in the coarse-grained fraction, which can be attributed to the source-rock types (Xie et al., 2020). Within the isotopically diverse Indus Delta sediment, the bulk isotopic compositions are estimated to deviate on average by no more than ±1.04εNd units and ±0.0099 for values in any sediment sample as a result of mineralogy, grain-size distribution, and analytical error (Jonell et al., 2018).
The εNd(0) signatures of the lithic fraction of sediments are taken as robust proxies of circulation and hydrologic processes because of their different origins across various timescales (Revel et al., 1996; Abbott et al., 2022). However, Sr–Nd isotope ratios in the lithogenic sediment fraction represent a complex mixture (Meinhardt et al., 2016; Bayon et al., 2021). The widespread influence of lithogenic neodymium on authigenic εNd(0) has been demonstrated. For example, there is a strong linear relationship between detrital εNd(0) and authigenic εNd(0) (r=0.86, n=871) (Abbott et al., 2022). Therefore, the sediment characteristics and detrital isotope records should be considered when using εNd(0) data. Different acid-leaching methods also have an effect on the Sr–Nd isotopic compositions of the silt and clay fractions in marine sediments (Walter et al., 2000). Acid-treated loess samples from the CLP and cryoconites (including surface dust) from high-mountain glaciers exhibit obviously higher ratios than samples without acid treatment and bulk samples (Rao et al., 2006; Nagatsuka et al., 2010, 2016).
Therefore, the provenance, grain size, lithogenic nature, and measurement methods of the Sr–Nd data from different media in this dataset must be considered when interpreting Sr–Nd isotope compositions in order to obtain good results.
3.2 The Sr–Nd data characteristics of glaciers at the third pole
Table 2 and Fig. 2 provide an overview of the information on samples from the third pole (the serial number of glaciers, subregions, glacier name, name of the sampling site where the samples were taken, sample type, sample age, sample elevation, and sampling longitude and latitude). The dust in snow and ice in the third pole originates from PSAs; therefore, the Sr–Nd data from these samples represent the characteristics of sinks. The Sr–Nd data from local or arid desert sand and soil represent the characteristics of PSAs. As an example, the isotopic signatures of the insoluble dust in snow and ice (sinks) at the third pole can be used to identify PSAs based on the data and geographic characteristics of sand and soil samples from the local exposed bedrock and distal arid deserts, from which dust is transported over long distances. Standard Sr–Nd measurement methods were applied to the snow samples (Xu et al., 2012; Du et al., 2015, 2019a; Dong et al., 2018; Wei et al., 2019, 2021), and standard measurement methods were applied to the sand or surface dust samples (Chen et al., 2007; Nagatsuka et al., 2010). The data results seem to remain fully consistent with these references.
On the basis of sorting criteria for determining PSAs based on the distributions of mountains and glaciers, geographic features, and isotopic values (snow or ice from the third pole glaciers, sand and soil from local and distal arid deserts), the third pole was divided into the following six isotopic subregions (Fig. 2):
Region I comprises samples from glaciers located in the Altai Mountains, including snow samples from Musidao Glacier and Altay as well as sand samples from the Gurbantünggüt Desert, with εNd(0) values from −6.6 to −1.2 and values ranging from 0.705483 to 0.71480. The highest εNd(0) values were observed in this region (Chen et al., 2007; Xu et al., 2012; Du et al., 2019a).
Region II comprises samples from the glaciers on the northern margin of the TP, including snow samples from the Tienshan Mountains (Tienshan No. 1 Glacier and Miaoergou ice cap) and Kunlun Mountains (Muztagata) as well as sand samples from the Taklimakan Desert, with εNd(0) values from −11.8 to −6.9 and values from 0.70842 to 0.728641 (Chen et al., 2007; Nagatsuka et al., 2010; Du et al., 2015; Xu et al., 2012; Wei et al., 2019).
Region III comprises samples from the interior of the TP. The Sr–Nd isotopic characteristics of the glaciers and sand/soil of this region include εNd(0) values ranging from −10.5 to −8.6 and values from 0.713192 to 0.721786 (Xu et al., 2012; Du et al., 2019a; Wei et al., 2021). Region IV comprises Sr–Nd isotope data from snow and sand/soil samples from glaciers in the Himalayan Mountains (East Rongbuk, Jiemayangzong, and Yala), with εNd(0) values ranging from −28.1 to −10.5 and values ranging from 0.724542 to 0.757407 (Xu et al., 2012; Wei et al., 2021).
Region V comprises samples from glaciers in the Qilian Mountains, including snow samples from the Qilian Mountains and sand (soil and loess) samples from the Hexi Corridor, with εNd(0) values from −15.7 to −7.0 and values from 0.712349 to 0.73211 (Wei et al., 2017; Dong et al., 2018). The εNd(0) values have an increasing trend along the Hexi Corridor from west to east. These trends are −15.7 to −12.9 for Laohugou No. 12 Glacier (local soil: −13.6), −13.7 to −8.58 for Qiyi, −13.8 to −13.6 for Shiyi Glacier (local soil: −13.8 to −13.6), −12.1 to −12.0 for the Dabanshan snowpack, and −10.9 to −7.0 for Lenglongling Glacier (Dong et al., 2018). It is very clear that, based on these local data, regional dust makes a significant contribution to these glaciers.
Region VI comprises samples from the glaciers in the eastern TP, including snow and soil samples from the Hengduan Mountains, with εNd(0) values from −17.1 to −10.1 and values from 0.717145 to 0.735863 (Xu et al., 2012; Dong et al., 2018).
There is an increasing trend from north (Region I) to south (Region V), and there is a decreasing εNd(0) trend from north (Region I) to south (Region V). The maximum ratios and minimum εNd(0) values were observed in Region V (Fig. 3). The Sr–Nd data in the third pole have relatively narrow ranges with distinct features, while the largest uncertainty was observed in Region IV (Fig. 3).
3.3 Sr–Nd data from the Arctic
Considerable Sr–Nd data have been obtained from modern snow and ice samples from the Arctic and surface (including sea-ice-transported sediments) sediment in the AO. These data cover the entire Arctic and represent the characteristics of a sink (Fig. 4). The data points are presented in Table 3. Sr–Nd data from arid deserts (East Asian and Saharan deserts) have been compiled in previous datasets (Blanchet, 2019; Robinson et al., 2021), and these data are useful for tracing terrigenous material transport in the Arctic. For user-friendly selection of the Sr–Nd data according to the modern environmental characteristics and the geographical location, Sr–Nd data from deep ice cores are not included in Fig. 5. We compared the Sr–Nd data from the surface snow (sink) and marine sediment (sink or source) samples in the Arctic (Figs. 5, 6). Based on the isotopic signals of these samples, geologic units, adjacent seas, and drainage basins of the main river systems in the Arctic, the Sr–Nd patterns can be divided into 12 subregions according to Maccali et al. (2018).
3.3.1 Sr–Nd data from snow/ice and sand samples from the Greenland ice sheet
Sr–Nd data from the East Greenland Ice Core Project (EGRIP) and the North GRIP (NGRIP) were obtained from snow pits. Sr–Nd data were also measured in the Greenland Ice Core Project (GRIP), the Greenland Ice Sheet Project 2 (GISP2), and the North Greenland Eemian Ice Drilling (NEEM) ice cores, and in the Renland, Site A, Hans Tausen, and Dye 3 shallow ice cores. The Sr–Nd data exhibit large differences in these samples (Fig. 5). The Sr–Nd data from NGRIP snow indicated that the dust sources were variable and showed complicated dust sources at the same location (Bory et al., 2002, 2003b). Much more Sr–Nd data have been recently measured from sand, soil, cryoconite, moraine, and englacial dust samples on the periphery of the GrIS (Nagatsuka et al., 2016). In these samples, the values are high, and the εNd(0) values are the least radiogenic (Table 3). Based on a comparison of the Sr data from the NGRIP and EGRIP snow pits (Bory et al., 2002, 2003b), much larger variations in were observed in the EGRIP snow pit, and lower values were observed in the NGRIP snow pit. The εNd(0) values in the interior of the GrIS were found to be relatively consistent, whereas large differences were observed at the periphery of this region. Therefore, although the Sr–Nd isotope ratios indicated that Asian deserts might be the main dust source for the GrIS, the ice-free region around the GrIS might be another source for the interior GrIS. In sediment samples collected from the Scoresby Sound region by Simonsen et al. (2019), the ratios range from 0.709689 to 0.736137, and the εNd(0) values range from −15.7 to −10.1. Based on a combination of the Sr–Nd values in snow (Renland, Site A, Hans Tausen, and Dye 3) and Dye 3 shallow ice core samples, as proposed by Lupker et al. (2010), the local dust sources may contribute some of the dust to the inland regions, and the Sahara is also the most likely additional PSA. The local dust from the ice-free areas of the GrIS may have been neglected in previous studies.
The mainstream view of the provenance of dust in inland Greenland deep ice cores (GISP2 and GRIP) is that the dust is from the eastern Asian deserts (the Gobi and Taklimakan deserts) based on the best Sr–Nd data matches during the last glacial period (Biscaye et al., 1997; Svensson et al., 2000; Újvári et al., 2015). High-resolution Sr isotope data from the Greenland NEEM ice core suggest that there was a significant Saharan dust influence in Greenland during the last glacial period (Han et al., 2018). The Sr–Nd data (>5 µm) in Holocene Renland ice cap project (RECAP) ice core samples are attributed to proximal dust sources; however, the resolution of the data is approximately 1000 years (Simonsen et al., 2019). Nevertheless, the Sr–Nd data in Greenland deep ice core samples (Biscaye et al., 1997; Svensson et al., 2000), which have low resolutions and represent multiyear averages with no seasonal or interannual variations (60 to 200 cm or 30–150 years), need to be considered when using some data.
3.3.2 Sr–Nd data from snow and sediment samples in the Arctic Ocean
Surface eolian dust from mid- or high-latitude continental weathering and arid deserts may be the most important dust contributor to snow and ice cores. The values are higher and εNd(0) values are lower in snow and sand samples from Ny-Ålesund, Svalbard (SV) (not including data from Iceland in Fig. 6). The Sr–Nd data in snow samples from sea ice were measured in bulk, and four of these samples were collected near the North Pole in the western AO by MOSAIC (October 2020) in this study (Figs. 4, 6). The εNd(0) data have highly negative εNd(0) values (−20.8 to −19.6), which cannot be explained by low-latitude potential dust sources. As shown in Fig. 6, the lowest εNd values were observed along the ice-free periphery of the GrIS and SV; therefore, these ice-free regions are potential sources of natural dust in the AO.
Terrigenous material from the Arctic marginal seas, including the Bering–Chukchi Sea (BCS), the Barents Sea (BS), the Canadian Arctic Archipelago (CAA), the East Siberian Sea (ESS), the Kara Sea (KS), and the Laptev Sea (LS), is transported to and deposited in the AO and may be the primary material source for marine sediment. The Sr–Nd data from Arctic surface sediments were based on the literature (Fig. 6), and most samples were sieved at <45 or 63 µm for bulk sediment samples. These samples were taken from the surface or from 0–10 cm from the surface in order to best represent the characteristics of coastal terrestrial sources, as presented by Maccali et al. (2018). The Sr–Nd values from the sediment samples (including sea-ice sediment) are almost the same as those of snow samples from the AO, indicating that the same PSAs exist in the central AO. The Sr–Nd signals in the sediment from the AO seem to be close to those from the BS, KS, and LS, which may indicate contributions from the Transpolar Drift originating over the Siberian shelves and crossing the AO towards the Fram Strait. The sample spatial coverage in each subregion is variable, and Fig. 6 shows the distinguishing characteristics of each region, but the Sr–Nd isotopic values overlap among close geographical regions to a great extent. Therefore, these data from different regions should be used carefully.
3.4 Information on Sr–Nd data from the SH and Antarctic ice sheet
By integrating the literature and adding data with new evidence, the dust provenances of low-elevation areas on the periphery of the AIS in the Holocene (including modern) are discussed. The dataset provides a comprehensive overview of the state of knowledge of dust sources and sinks in different sectors of the AIS and PSAs in the SH. The location of Sr–Nd datasets from different sectors of Antarctica and the AIS are presented in Fig. 7. The Sr–Nd data from Antarctica are not evenly distributed, and more data have been measured in western Antarctica and the Ross Sea. The Sr–Nd data from PSAs in the SH (Australia, SSA, and SA) clearly reflect the characteristics of these regions and provide insight for tracing dust source–sink paths. For example, the ratios in Australian dust samples range from 0.709 to 0.732, and the εNd(0) values are between −15 and −3 (Revel-Rolland et al., 2006). The Nd values from Patagonia (39–52∘ S) in SSA are more radiogenic (−1 to 1 for εNd(0)) (Gaiero et al., 2007). The eolian dust from Argentina and Chile is confined to the ranges of and −5<εNd(0)<3 (Delmonte, 2003). The ratios in the sand samples from SA vary between 0.712348 and 0.74716, and the εNd(0) ratios vary between −24.5 and −8.4 (Delmonte, 2003; Gili et al., 2022). These Sr–Nd data can very clearly distinguish geographic subgroups of PSAs in the SH.
3.4.1 Sr–Nd data from sediment from Antarctica
The Sr–Nd data from the marine sediment (near-core-top samples) from the circum-Antarctica region and terrigenous materials (eolian dust, glacial drift, and dust in ice core) from the AIS are presented in Fig. 8. The ages of these samples were limited to the Holocene. We compared these data with PSA samples from the SH. At some sites, with >2 samples, we plot the average Sr–Nd values on the map. For example, the values range from 0.705281 to 0.725643 in the Pacific sector (146.78∘ E–67.27∘ W), 0.710616 to 0.738862 in the Indian Ocean sector (20.00–146.78∘ E), and 0.715989 to 0.741609 in the Atlantic sector (67.27∘ W–20.00∘ E) (Hemming et al., 2007). In Fig. 8, the Sr and Nd isotopic contours were determined by inverse distance-weighted interpolation, and the number of data points were >2 at some sites. At such sites, the average of the surface samples was obtained. The patterns of the two isotopic compositions are consistent across the AIS. Although the values differ between sediments from the circum-Antarctic region and sand from PSAs (Australia, SSA, and SA), the and εNd(0) patterns from the Pacific sector and the Indian Ocean sector are relatively consistent with those from SSA and SA, which can be partly explained by the contribution of eolian dust to the entire SO. It seems that the Sr–Nd values found in the Ross Sea and Amundsen Sea are anomalous, which may be attributed to the much greater number of samples collected in the two regions.
3.4.2 Sr–Nd data on the periphery and interior of the Antarctic ice sheet
New Sr–Nd data from coastal and low-elevation sites were measured in ice-free areas near the Filchner–Ronne Ice Shelf, Ross Ice Shelf, and Amery Ice Shelf (Fig. 7). The Sr–Nd isotope compositions of four sand samples from southern King George Island (South Shetland Islands) in West Antarctica were characterized by less-radiogenic values ranging from ∼ 0.703907 to ∼ 0.704157 and relatively high εNd(0) values ranging from 4.6 to 6.4. The ratios ranged from 0.71135 to 0.72377, and the εNd(0) composition ranged from −13.3 to −9.6 in ice-free areas of Inexpressible Island in the Ross Sea, West Antarctica. Based on our own Sr–Nd data and the literature (Table 3), we observe the highest εNd(0) value of >−5.0 in McMurdo and King George Island. There are large variations in values and moderate εNd(0) values in Victoria Land and the Ross Sea (including Inexpressible Island). The Amery Ice Shelf features high ratios as well as the lowest εNd(0) values of <−15. These subregions are very close to the εNd(0) data from the different sectors of circumpolar sediments (Roy et al., 2007). Therefore, the dataset will be useful for tracing the dust sources and sinks in the SO and AIS.
However, because the Sr–Nd data differ significantly among some of the regions and are similar among others, care must be taken when directly comparing these data to precisely explain the observed isotopic compositions in ice core records. For example, there is overlap in the Sr and Nd isotopic compositions of King George Island, SSA (Patagonia), and the McMurdo dry valleys. The Sr–Nd data from Inexpressible Island also overlap with the other end-members (SA, New South Wales, and Prydz Bay). Therefore, dust from low-latitude regions (New South Wales and SA) cannot be excluded from East Antarctica (Du et al., 2018; Gili et al., 2022). Another example is the characteristics of snow layers of the Berkner Island ice sheet in western Antarctica. These data can be partly explained by the surface sediment samples from the Weddell Sea sector, with εNd(0) values ranging from −10 to −8 (Hemming et al., 2007). Therefore, the dataset from the SH and AIS demonstrates that multiple mixed sources can be inferred from Antarctic surface snow samples. However, among the data from the entire AIS, the Sr–Nd isotopic components were measured in only 29 snow samples, and there is an urgent need to collect more data in the future.
Information on Sr–Nd data in Antarctic ice cores during the Holocene and glacial–interglacial times is presented by integrating the literature (Du, 2022). To obtain enough dust particles, samples with different age intervals were merged. For example, each sample represents approximately 40–160 years for the Vostok ice core, which may cover about a few thousand years to obtain a single large-volume sample (Delmonte et al., 2008). Alternatively, several ice core sections from different depths were integrated to obtain a few large samples for the Sr and Nd isotope analyses of the Talos Dome ice core (Delmonte et al., 2010b). A relatively high resolution (spanning between ∼ 3 and ∼ 30 years) was used in the Taylor Dome ice core (Aarons et al., 2016). Sr–Nd data in the Antarctica deep ice core mainly focus on the coastal and inland areas of the EAIS. As previously mentioned, the dust source is similar to that of the modern samples in the Dome C and Vostok ice cores during the Holocene and interglacial periods, which can be explained by an SSA provenance; an additional hypothesis explains the isotopic signature of Holocene dust in central East Antarctica (Delmonte et al., 2008, 2019). Sr–Nd data from the Talos Dome, Taylor Dome, and Taylor Glacier ice cores during the Holocene point towards a local dust provenance (Delmonte et al., 2019; Aarons et al., 2016, 2017). Therefore, the Sr and Nd data from East Antarctica ice cores during the Holocene and interglacial periods indicate a well-mixed atmospheric background involving a mixture of two or more sources in the SH (Fig. 8). The study demonstrated that SA emerges as the second most important dust source for East Antarctica during interglacial periods (Gili et al., 2022).
However, samples from glacial stages (stage 4 at ∼ 60 ka and stage 6 at ∼ 160 ka) in the Vostok ice core span a very narrow range of Sr compositions () and Nd compositions (1.1<εNd(0)<5.0), which can also be explained by the Sr–Nd data in sand samples from southern King George Island ( values ranging from ∼ 0.703907 to ∼ 0.704157 and εNd(0) values ranging from 4.6 to 6.4). The and εNd(0) isotopic compositions of dust in the Taylor Glacier ice core samples during the last glacial period indicated that dust may have originated from SSA and from potential local source areas in the Ross Sea sector (Delmonte et al., 2010b; Aarons et al., 2016, 2017). Therefore, these data suggest that the glacial-period dust in East Antarctic ice cores also features local contributions. However, almost no Sr–Nd data were obtained from West Antarctic deep ice cores, which limits our understanding of the spatiotemporal characteristics of dust transport across the entire AIS. More importantly, the ages of the Sr–Nd data from surface eolian dust from the AIS and PSAs in the SH are unknown, which hinders accurate dust source or sink tracing.
All datasets and the associated metadata table presented in this study are available from the Big Earth Data Platform for Three Poles. The dataset can be downloaded from https://doi.org/10.11888/Cryos.tpdc.272100 (Du, 2022). In this repository, all datasets are provided in Excel spreadsheet format along with metadata files.
An integrated Sr–Nd dataset for the remote three poles is presented, and these data were not easily collected because of the extremely cold and high-elevation environments. The dataset is complicated and includes snow, sand, soil, loess, deposits, sediment, and other sample types. We present case studies of snow, ice cores, and sediment samples to demonstrate the Sr–Nd characteristics of the third pole glaciers and Arctic and Antarctic ice sheets. These integrated data can provide a new perspective on present and paleodust sources and sinks at the three poles and, more importantly, clearly emphasize the following points for potential users of the datasets provided with this paper:
This Sr–Nd dataset enables us to map sampling locations in the remote three poles, while the use of sorting criteria related to the sampling location, type, or resolution permits us to trace the dust sources or sinks based on isotopic signatures.
For the third pole, the Sr–Nd isotopic data were divided into subregions, and the integration of these data from sand/soil and snow samples in six subregions allowed us to clearly understand the Sr–Nd data characteristics of the third pole. These data will be useful for users seeking to trace the local or long-distance-transported dust from the source to the sink.
The Sr–Nd characteristics in snow/ice and sediment samples show that there are significant differences among the different subregions in the Arctic, which will be useful for tracing dust sources and sinks
The new data from Arctic and Antarctic samples emphasize that the ice-free regions on the periphery of the ice sheets may be important local dust sources. However, there is Sr–Nd data overlap in the low-latitude regions in Antarctica, and the paucity of data in Antarctica is severe; thus, future studies should concentrate on this aspect.
CX, ZD, and AS designed the study. ZD, JY, CX, and AS wrote the manuscript. ZD, LW, NW, SW, and YL collected the samples in the field and produced the data. ZD, NW, LW, SW, YL, ZZ, JX, and XM performed the analysis. All authors contributed to the final form of the paper.
The contact author has declared that none of the authors has any competing interests.
Publisher's note: Copernicus Publications remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
This article is part of the special issue “Extreme environment datasets for the three poles”. It is not associated with a conference.
We thank everyone involved in the snow sample collection from the central Arctic Ocean, within the framework of the RV Polarstern expedition, for their great logistical support during MOSAiC in 2019–2020. We also thank the Chinese Arctic and Antarctic Administration for their contribution to MOSAiC.
This research has been supported by the Strategic Priority Research Program of the Chinese Academy of Sciences (grant no. XAD19070103), the National Natural Science Foundation of China (grant nos. 42071086 and 41971088), the State Key Laboratory of Cryospheric Science (grant no. SKLCS-ZZ-2022), and the Youth Innovation Promotion Association of the Chinese Academy of Sciences (grant no. 2020419).
This paper was edited by Xin Li and reviewed by Cecile Blanchet and two anonymous referees.
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