Introduction

Glass waste forms are required to safely dispose of radioactive waste by immobilizing radionuclides and mitigating their release into the environment. At the Hanford site, a Department of Energy legacy nuclear waste site in Washington state, USA, hundreds of thousands of cubic meters of legacy radioactive waste from plutonium production will be immobilized in glass, with low activity waste (LAW) glass disposed in a near-surface integrated disposal facility (IDF). As described elsewhere1, LAW glass will be prepared using a vitrifying supernatant and saltcake from the Hanford waste tanks. The glass must limit radionuclide release to the environment for thousands of years, which is challenging to assess in laboratory experiments. Central to radioactive waste management is a detailed understanding of the corrosion processes and a quantification of the corrosion rates of the glass waste form. However, laboratory glass corrosion experiments have a limitation: their timeframes are considerably shorter than the timeframes over which radionuclides must be retained in a nuclear waste disposal site. Studies of natural analogs2,3,4,5,6,7,8,9,10 and anthropogenic glasses from archeological sites11,12,13,14,15,16 can help bridge this important gap. Using such glasses has significant theoretical and practical implications for nuclear waste management. By validating models used to assess waste form behavior with findings from natural and anthropogenic glasses, we can better understand the long-term performance of nuclear waste glasses. The alteration environments for these glass analogs vary in terms of temperature, pore fluid chemistry and pH, solid surface area to liquid volume ratio, percolation rate, and soil microbial communities. These variables must be considered when comparing analogs with proposed nuclear waste glasses10.

Natural glass analogs, such as basaltic glasses (45–50 wt.% SiO2), tektites (65–90% wt.% SiO2), and obsidian glasses (70–75 wt.% SiO2), are found in terrestrial environments. The thickness of the surface alteration layer (referred to as “palagonite“) can be used to semi-quantitatively evaluate the alteration rate of such natural glasses16,17. Research suggests that the alteration mechanisms of natural, anthropogenic, and nuclear glasses are similar7. As an example, Techer et al.17 compared the alteration of basaltic glass (ages ranging from several thousand to a few million years) in natural environments with the alteration of basaltic glass and a reference nuclear waste glass (SON68) under laboratory conditions for periods of 4 days up to several hundred days. These authors pointed out some uncertainties and assumptions for natural samples, for example, the uncertainty in the nature of the altering environment and glass-solution contact time, and the assumption that the palagonite thickness can be directly compared to alteration layer thicknesses measured on glasses corroded in laboratory experiments. However, the results suggest that the mean alteration rate estimated from measured palagonite thicknesses was comparable to rates measured in closed system laboratory experiments for high reaction progress17.

Archeological glasses have also been used as analogs for comparison with alteration behavior predicted by nuclear waste glass models18. While archeological analogs are not compositionally identical to natural and nuclear glasses, they do contain most of the same major elements (alkalis, Si, Al, Fe, etc.)19. Archeological glasses also meet the criteria for an analog because information about the altering environment over the glass’s exposure time is often well documented. For example, two Roman glasses have been used as analogs to study long-term glass alteration behavior: (1) glass from a shipwreck off the coast of Embiez Island, France13,14,15; (2) glass from the shipwreck Iulia Felix off the coast near Grado, Italy12,20,21. These two glasses with similar compositions were altered in marine environments for nearly 1800 years. The Embiez glass was altered in open water in the Mediterranean Sea (15 °C). The Iulia Felix glass was altered in the Adriatic Sea (15 °C), which has a slightly different chemistry than the Mediterranean, and was covered with sand during its alteration. The Embiez glass shows significant cracking due to fast cooling during its fabrication, and an alteration behavior that is dependent on the size and the locations of the cracks13. The same cracking phenomenon is observed in nuclear waste glass fabrication. The glass from the Iulia Felix shipwreck contains both colored20 and colorless fractions21. The two glass fractions have compositions that vary only slightly; however, alteration of the colorless fraction results in an opaque white crust, mainly composed of silica (SiO2), while the colored fraction shows alteration layers consisting of repeating lamellae22. Lamellae have also been observed in static tests of nuclear waste glass at acidic (pH = 4.1) conditions23. This type of alteration has not been observed in laboratory testing at pH values near those expected in a disposal facility (pH 6–9), but the pH-dependence of lamellae formation needs to be confirmed24. Wang et al.25 have proposed that lamellae formation can be explained from a positive feedback between dissolution-induced cation release and cation-enhanced dissolution kinetics.

Waste glasses are typically subjected to short-term, accelerated laboratory tests to demonstrate that they are chemically durable for long periods. The kinetic behavior of these accelerated laboratory tests is then extrapolated over long time periods, but may not yield accurate predictions of glass durability over thousands of years. In addition, glass analogs have been used to predict the alteration of nuclear waste glasses during disposal in subsurface geological repositories6,9,10,19. In particular, natural and archeological glasses can be used to assess how the alteration layers on the glass may have formed in response to near-field environmental conditions.

In this study, we characterize natural and archeological glasses from five near-surface sites exposed to different environmental and climatic conditions (e.g., average temperatures, extent of hydraulic saturation, etc.). A detailed description of the sites is provided, along with characterization data for the excavated samples. The range of environmental conditions these sites cover is relevant to the disposal of radioactive LAW glass at the near-surface, hydraulically unsaturated IDF Hanford site.

Unlike highly radioactive material, which will be buried deep underground in stable rock formations in a geological disposal facility, low activity radioactive waste does not require shielding and is suitable for disposal in shallower facilities closer to the surface. The Integrated Disposal Facility (IDF) is intended to be a near-surface disposal facility for radioactive LAW glass at the Hanford Site (Figs. 1 and 2A). It is a large, lined disposal trench excavated ~13 m deep into the Hanford sands in the Central Plateau at the Hanford Site. The key engineered design features of the IDF consist of: (1) containers around the waste and a surface barrier placed above the waste containers to limit contact with water; (2) engineered backfill placed between and above waste containers to provide structural support after closure; (3) borosilicate glass waste forms that limit the release of contaminants due to the slow dissolution of the glass matrix. The key natural features consist of: (1) a semi-arid climate and shrub-steppe ecology that results in minimal natural recharge to the groundwater due to low annual precipitation rates and high evapotranspiration; (2) a thick vadose zone that delays the time it takes contaminants released from the source term to arrive at the saturated zone. At the Hanford Site, basalt is underlain by Tertiary continental sedimentary rocks and overlain by late Tertiary and Quaternary fluvial and glacio-fluvial deposits. The climate at the Hanford Site is mid-latitude semiarid desert. Daytime high temperatures in June, July, and August range from 17.2 °C to 27.9 °C but can exceed 40 °C. During the winter, temperatures generally range from −0.2 °C to 6.9 °C but can occasionally drop below –18 °C. The typical annual relative humidity is 54%, and the average annual precipitation is ~180 mm, with about 38% as snow26,27. At Hanford, winters are projected to be wetter and summers drier, with temperatures estimated to rise 1.7–5.6 °C this century, continuing the 0.83–2.2 °C rise from last century27,28. The precipitation is expected to range from −10% to +20% from current levels to ~208029. The Hanford Site experienced massive glacial flooding ~13,000 years ago as the last Ice Age was ending. Temperatures rose 2.8 °C, and the climate became substantially (up to 50%) drier than today27,30. The Hanford site has undergone considerable change in the last 100,000 years; annual precipitation ranged from 50−128% of present-day levels, with a −2.5 °C to 2.8 °C range in annual temperature27,30. The future climate of the Hanford site is expected to be as variable as it has been in the past26,27.

Fig. 1: A schematic of the Integrated Disposal Facility (IDF) in the Central Plateau at the Hanford site.
figure 1

The view is a cross-section of the facility, and the dimensions are for information only.

Fig. 2: Location of natural and archeological analogs sites.
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A Hanford IDF, near Richland, WA, USA, B Newberry Volcano (Big Obsidian Flow), near Bend, OR, USA, C Ballidon Experiment Site, Tarmac Quarry, Derbyshire, UK, D Broborg Hillfort, Uppland, Sweden, E Dobkowice Archeological Site, Subcarpathian Voivodeship, Poland, F Timna Site (Slaves’ Hill), Timna Valley, Israel. The overview image was created using ESRI ArcMap; all others were created using Google Earth.

To establish limits on radionuclides that will be disposed of in the near-surface IDF, an assessment of impacts to groundwater resources must be made so that the concentration of radionuclides does not exceed the current drinking water standard. The assessment established a 1000-year compliance evaluation with additional analysis performed out to 10,000 years to determine peak elemental release31. To make this assessment, the alteration behavior of the LAW glass in the near-surface environment of the IDF must be known.

Samples were chosen from specific analog sites to evaluate the following parameters: (1) how variation in surficial geology affects glass degradation; (2) effects of the environment on glass degradation; (3) comparison of sites with respect to the geology and current environment conditions, and possible environmental changes at the IDF; and (4) effect of hydraulic saturation (especially compared to the nominal conditions at the IDF). Several of these analog glasses are from archeologically significant sites, therefore, it was not possible to randomize sample collection. This resulted in an unintentional bias towards sample types that were more widely available for characterization. The site characteristics, as detailed below, vary in terms of (1) the amount of time the glass was buried, (2) the chemical composition of the glass, (3) the surficial geology, (4) the environment (precipitation and climate), (5) burial depth, and (6) site elevation. Table 1 summarizes the analog glasses chosen for study, Fig. 2 provides a map of the excavation sites, and Fig. 3 provides a timeline comparing relevant timescales (the alteration timescales for the analog sites will be described in the subsequent sections). Information on the geologic setting for each site is available in the supplementary materials.

Fig. 3: Timeline showing relevant time periods and ages of analogs, redrawn from Weaver et al.102.
figure 3

For sites with analogs from multiple time periods, a colored rectangle describes the minimum and maximum ages. The timeline is shown in years before present, with present defined as 2024. For nuclear waste disposal, glasses are assessed for a 1000-year compliance evaluation with additional analysis performed out to 10,000 years to determine peak elemental release31.

Table 1 Summary of glasses and alteration environments

The Broborg site (59°45’20” N, 17°57’06” E, elevation 49 m) Viking hillfort (Fig. 2E) was established ~ 375–550 CE19 in what is now the southeastern Uppland Province, ~25 km southeast of Uppsala. The technology and materials used to construct this hillfort are summarized by Sjöblom et al.32. Vitrified rock samples were collected from the Broborg site during multiple excavations (1982–1983, 1990 and 2017) and are described elsewhere33,34. Bulk sample analyses of the granite and amphibolite rocks were presented by Ogenhall35. Vitrified materials from the Broborg site were produced when the local amphibolite and granite were melted in situ32,36,37,38. The vitrification of the amphibole-rich rock produced a dark Fe- and Mg-rich glass, while the vitrification of the granite yielded a clear Na- and Si-rich glass. The altered layers observed on excavated samples were compared to altered layers observed on excavated material that had been remelted to form coupons, which, in turn, were subjected to laboratory testing (vapor hydration test, VHT, product consistency test, PCT, and EPA method 1313)16.

Broborg’s selection as an analog site provided an opportunity to study ancient glass buried in a soil that is a mixture of ancient mountain soil and more recent till-derived sandy clay loam39. The overall climate of this site can be characterized as relatively humid and continental. Before the hillfort was constructed, temperatures were slightly warmer than the long-term average in the Roman Warm Period40 (Fig. 3). When the fort was active, the Dark Age Cold Period (ca. 300–800 CE) was marked by temperatures below the long-term average40. Volcanism in Iceland caused temperatures to plummet from 536 to 539 CE41,42. The Medieval Warm Period saw an increase of 0.3 °C to 1.1 °C compared to the local maximum. After the maximum, another cooling trend occurred during the Little Ice Age (LIA) before reversing around 1600 CE with warming to 2000 CE40,43.

The Timna site (Fig. 2F), situated in the Aravah valley of the southern Negev desert (Israel), is known for its well-preserved historic copper mining districts that reveal at least 7000 years of archeological evidence of metallurgical activity. The region’s tectonic and hydrothermal activities, combined with the local lithologies, contributed to the formation of copper deposits44. Ancient smelting sites provide evidence for copper production from the Copper Age to the Early Islamic Period. The vitrified slag samples from Timna described in the present paper were retrieved from copper smelting sites from the Early Bronze Age to the Early Islamic Age45. Timna’s primarily hot desert climate and arid soils contrast starkly with those of the other analog sites. The dominant soils in Timna are aridisols46,47. These are dry soils with limited organic matter and weak soil structure. Due to low rainfall and high evaporation rates, they are often saline46,48,49. Due to the limestone and chalk bedrock in regions around Timna, some soils exhibit a high calcium carbonate content, which can form hardpans or caliche layers50.

Hyper-arid conditions have dominated the Aravah Valley since the late Pliocene and early Pleistocene51,52,53 due to it being located in the rain shadow of the Negev Highlands52,53,54. The middle Holocene experienced significant climate fluctuations, ranging from hyper-arid periods to intervals with higher levels of precipitation51. This was superseded by drier conditions with fewer oscillations in rainfall in the late Holocene. In the Middle Bronze Age to the end of the Late Bronze Age, humidity increased, followed by a sudden and pronounced ~150-year dry event occurring from 1300 to 1200 BCE51. The late Iron Age was marked by increased aridity encompassing the Near East52,54. Climate change has impacted Timna in the modern era. The twentieth and twenty-first centuries have seen a general trend of increasing temperatures, with precipitation patterns becoming more unpredictable and extreme55.

The Newberry Volcano, near Bend in central Oregon and east of the Cascade Range on the western edge of the High Lava Plains, is one of the largest and most active volcanoes in the contiguous United States. Samples were collected in 2021 from Newberry’s Big Obsidian Flow (BOF) (43°41’36” N, 121°13’45” W, elevation 2206 m) (Fig. 2B). Newberry last erupted ~1350 years ago (i.e., ~675 CE), resulting in the BOF56,57,58,59. The obsidian from the most recent flow contains 72.8 wt.% SiO256 and differs from most other rhyolitic rocks on the Newberry volcano in its much higher Rb/Sr ratio57.

Newberry samples were chosen for this study due to their natural origin, unique chemical composition, and climate. The soils that contact the BOF are andisols. They are primarily derived from volcanic materials and tend to have a loamy texture with a balance of sand, silt, and clay, thereby allowing good water infiltration and root penetration60. During the Medieval Climate Anomaly (MCA), the Newberry region experienced warmer and drier conditions61. During the LIA, cooler temperatures prevailed, with more frequent and extended wet periods influencing the region’s ecosystems and human settlements62. Following the LIA, temperatures at Newberry and the overall Pacific Northwest region began to rise. The twentieth and twenty-first centuries have seen an acceleration of this warming trend, consistent with global climate change patterns. Recent studies have shown a decline in snowpack levels in the Oregon Cascades and a trend toward earlier spring snowmelt56,57,63.

Dobkowice is a town in Jarosław county of Poland’s Subcarpathian province, situated on the northern edge of the Carpathian Foredeep geological basin. Approximately 30 glass beads and other artifacts from the Bronze age were excavated from a crematory gravesite (49°55'48.92” N 22°42'55.85” E, elevation 218 m) (Fig. 2E)64. The glass beads were made using a mixture of natron and lime/shells with sand65. Because of their soda-lime-silica composition, these glasses are commonly referred to as natron glass or low magnesium glass (LMG). The beads, relics of the Jordanów culture, are estimated to be ~2600 years old (i.e., ~430 ± 150 BCE) and vary in color from light green to light brown64. A local farmer discovered the site in 1971 a few hundred meters northwest of the town. Excavations were conducted in the 1970s and 1980s, and finally in 2011–2012 before construction of a highway began66,67. The Dobkowice site offers an opportunity to investigate anthropogenic glass buried in saturated soil in a relatively wet environment. The soil of the Dobkowice archeological site is an eutric fluvisol (soil base of saturation >50%)68.

During the so-called Roman Warm Period (RWP) period (Fig. 3), Poland, along with the rest of Europe, likely experienced warmer climates69, with relatively colder and drier winters offset by warmer and wetter summers70. After the RWP, a cold period that lasted until about 800 CE brought cooler temperatures. During the last ~1000 years, until 1860 CE, summers and winters were colder than in previous millennia70. The MCA, or Medieval Warm Period, was characterized by a warmer phase with temperatures that may have resembled modern pre-industrial times (Fig. 3)61. During the LIA, Poland and its surrounding areas experienced significantly colder winters and summers, which profoundly affected agriculture, settlements, and even warfare71. Post-LIA warming was observed in Dobkowice and the surrounding region. In the twentieth century, warming accelerated due to anthropogenic factors72. In recent decades, Poland has experienced higher temperatures, changes in precipitation, and increased extreme weather events such as heat waves and heavy rains, with an overall trend of rapid warming73.

The Ballidon quarry site offers a controlled environment allowing the study of both natural and anthropogenic glasses. The Ballidon glass burial experiment (53°05’38’N, 1°42’08” W, elevation 228 m) (Fig. 2C) was initiated in 1963, based on preliminary results from buried glass samples from the Experimental Earthworks in Wareham74. Various glasses were buried, including replicas of Roman soda–lime–silica glass, potash–lime–silica circa seventeenth century, and medieval glass75,76. The pore water pH conditions at Wareham were acidic (pH 3.8–4.7), so the degradation of the glass samples was less representative of disposal conditions. Glass samples were more recently buried at Ballidon and experienced an alkaline (pH 7.8–8.2) limestone quarry environment74,76,77. At Ballidon, samples were placed in a burial site originally measuring 3.5 m × 1.5 m and covered in limestone fragments, comprising pieces of crushed limestone (1 cm–8 cm fragments of calcite). At a sample depth of <20 cm, samples may occasionally have been affected by severe frosts. The soils at the Ballidon are loamy brown peaty top soils underlain by clay subsoils, with an average pore water pH of 9.678,79. Over the past 50 years, Derbyshire’s climate has become slightly warmer and wetter, paralleling broader climatic trends across the UK74,76. According to the UK Meteorological Office, the average temperature in the UK increased around 0.8 °C between 1961–1990 and 1991–202080,81. This increase was most substantial in central and eastern England, where some areas saw temperatures rise by more than 1.0 °C80,81. Despite elevated precipitation conditions, there are intermittent drying periods during the summer months. These fluctuating environmental conditions, as compared to other disposal sites, may be responsible for their unique alteration signatures76.

The experiment was initially planned to run for 512 years, with the extraction of samples from sites within the mound at increasingly-spaced time intervals: 1, 2, 4, 8, 16, 32, 64, 128, 256 and 512 years74. The 64-year sample retrieval was brought forward in time due to interest in nuclear waste-form glasses. From 1986 onwards, simulant nuclear waste glasses, including glass formulations from the UK, USA, and Russia, have been buried in vacant sites at Ballidon for various periods of time.

Similar glass burial experiments have also been undertaken elsewhere, including Chalk River Nuclear Laboratories (CRNL) in Ontario, Canada (1959–1978)82, the Stripa granite mine, Sweden (1982)83, the Boom clay in Mol, Belgium (1986)83, the halite disposal facility at the waste isolation pilot plant (WIPP) at Carlsbad, New Mexico (1986)84, and the Hanford lysimeter site (present day) in glacial lake deposits and gravel85. To directly compare the effects of local environmental factors on glass alteration, the same simulant nuclear waste glasses have been buried at the Stripa, Mol, Ballidon, Carlsbad, and Hanford sites83. A discussion of other near-surface burial sites is provided elsewhere86.

Results

Analyses were performed on analog samples from the five sites, and results are discussed in terms of the chemistry of the analog glasses, followed by observations and measurements of the surficial alteration layers prepared in cross section (or in the case of the Dobkowice sample, one set of images was taken along the as-cut surface without mounting in resin or polishing). Table 2 provides measured bulk compositions for samples from the five sites. These bulk compositions were measured using either EPMA, or ICP-OES and ICP-MS following chemical digestion.

Table 2 Comparison of select site sample compositions (wt%)

Timna

For the samples that were excavated from Timna, the twelve samples chosen for analysis were biased toward material with high glass contents. These 12 analogs include 11 glassy slag samples and one tuyère sample (the Timna-L sample) that were taken from three smelting sites in or near the Timna Valley: site 28, site 34, and site 201. The tuyère sample (Site 34) is approximately 3150 years old87. The tuyère was a ceramic nozzle forming part of the bellows that were placed inside the furnace, usually pointing down to direct a forced draught towards the lower charcoals. The tuyère withstood extreme heat inside the furnace, with the surrounding area reaching temperatures of approximately 1300–1500 °C, allowing for molten metallurgical slag to accumulate on the tuyère, which mostly vitrified on cooling88. Site 28, named the Be’er Ora “Slag Valley,” was a big smelting camp located south of Timna Valley. Radiocarbon dating of samples from site 28 found that these materials mostly dated to the seventh to tenth centuries CE89,90,91. Site 34, named “Slaves Hill,” has been a key site of the Central Timna Valley (CTV) project, which has been led by researchers from Tel Aviv University. It was excavated between 2012 and 2023 and has received the most attention of all Timna sites. Radiocarbon dating revealed that smelting occurred roughly between the late eleventh and tenth centuries BCE87. Site 201 is located on top of a small hill on the western side of the Aravah, just 5 km north of Timna Valley. The CTV Project excavated Site 201 in 2020 to further understand technological developments associated with the very early history of extractive metallurgy. Radiocarbon dating suggests that the site was active at several periods, from the end of the late Copper (4000 BCE) to the Early Bronze Age.

Table 3 compares the amorphous contents of 12 Timna samples determined by XCT and XRD (using semi-quantitative Rietveld refinement) and lists the approximate ages of the samples. Figures 4 and 5 show XCT reconstructions and optical micrographs of 12 Timna samples, while Fig. 6 shows the corresponding XRD patterns. Overall, the more recent samples exhibit larger amorphous contents, which is attributed to improvement in the melting technology with time, leading to faster heating and cooling rates in the furnace.

Fig. 4: XCT reconstruction of Timna samples showing internal structure.
figure 4

Three-dimensional XCT reconstructions of 12 Timna samples (AL). The greyscale values in the individual images represent the relative attenuation of X-rays, which is a function of mass density and show the distribution of inclusions and voids within the samples.

Fig. 5: Optical microscopy images of 12 Timna samples showing physical appearance for comparison with XCT data on internal features.
figure 5

Optical microscopy images of 12 Timna samples (AL).

Fig. 6: XRD patterns of Timna samples to assess phase distribution and amorphous Content.
figure 6

The XRD patterns of Timna samples (AL) are shown after addition of a 5 wt.% CeO2 internal standard. In the figure: Q-quartz (SiO2), Fy- fayalite (MgxFe1-x) SiO4, D-diopside (MgCaSi2O6), and Bbirnessite (MnO2·nH2O).

Table 3 Comparison of amorphous contents (measured by XCT and XRD) and sample ages for 12 Timna samples

All the Timna samples show a thin surficial discoloration assumed to be an alteration signature. The surficial layer on the tuyère sample, which is a sample containing a large glass content, is not visible along the entire surface, but has a consistent thickness in the regions where it is observed. Figure 7 shows a ~2 µm thick surficial layer on a Timna sample obtained using SEM. The back-scattered electron (BSE) image shows heterogeneities in mass density within the layer, which are particularly noticeable when compared to the uniform, unaltered bulk material. Silicon shows no major change in concentration, whereas Mg is enriched in the layer. The interfacial gradient in the Mg concentration, at the scale of the image, is relatively sharp. The bulk material does show a few white circular regions, whose origin is not known. It is interesting that these circular areas are enriched in Cu and depleted in Si. The BSE image also reveals the presence of a very thin dark band at the inner boundary between the surficial layer and the bulk, discussed in the next paragraph.

Fig. 7: Optical and electron microscopy of Timna-L sample showing surficial layer.
figure 7

Comparison of: A Optical microscope image of partially vitrified Timna-L sample. B, C SEM-BSE (backscattered electron) images of partially vitrified sample showing scale of surficial layer (denoted as “SL” in C). In B, a red arrow points from the approximate location of the elemental map shown in (C).

Figure 8 shows the same area measured by ToF-SIMS. The elemental maps show that the surficial layer has a constant thickness (~2–3 µm) and is enriched in H, Mg, Al, Si, K, and Cu (Cu just slightly), and depleted in Na and Ca. All enriched elemental maps (including Ca) display some heterogeneity, characterized by small, localized areas with higher-than-average concentrations. The surficial layer has an additional and extremely thin but non-continuous external layer that shows even higher enrichment in Mg, Al, Si, and K. This very thin layer is also evident in the SEM-BSE image of Fig. 8. Both the chemical maps and the BSE image show the same thin band at the inner boundary that separates the surficial layer from the bulk (Fig. 7). This black band may point to a physical gap, suggesting that the layer is not strongly bound to the bulk material.

Fig. 8
figure 8

ToF-SIMS maps of partially vitrified Timna-L sample and the corresponding SEM-BSE image of the same area.

Ballidon

Here, results are presented for a replica medieval glass sample (of potassium-lime-silica composition, designed to replicate a specific glass known as the “Hangleton linen smoother”92) that was excavated from the Ballidon experimental mound76. This sample was altered under near-surface conditions for a duration of 52 years before retrieval. The sample was mounted in epoxy, polished, and analyzed using EPMA. Figure 9 shows SEM-BSE images and elemental maps of the surface layer (SL) of the replica medieval glass sample. After 52 years, the alteration layer on this sample is considerably thicker than those on the Timna samples, ranging from 400 µm to 1000 µm. The SL is not homogeneous but appears to change abruptly in the sub-layer adjacent to the soil, with respect to the presence of gaps or pores between the much thinner layers. The elemental distributions of the various elements show an alternating pattern of bands corresponding to element depletion and enrichment. The SL, furthest from the pristine glass, appears more chemically separated (“banded“) whilst the younger alteration next to the pristine glass appears more uniform. The bands of enrichment and depletion also appear to be anti-correlated. The bands enriched in Al, Si, and possibly K are spatially correlated with the same bands showing depletion in Ca, P, Fe, and Mg (panel C). The chemical boundaries of the bands are relatively sharp, except for Na and K, which are in part indistinct. The band widths vary in thickness (10–25 µm), which is particularly evident in the Fe, Si, P, and Ca maps. Such banding was also present in the Roman glass from the Iulia Felix shipwreck21,93,94.

Fig. 9: Analysis of surficial layer on replica medieval glass sample from Ballidon.
figure 9

A SEM-BSE image, B higher magnification SEM-BSE image and C EPMA-WDS maps of a replica medieval glass sample excavated from the Ballidon site showing a surface layer (SL) with prominent depletion-enrichment banding. Approximate SL-bulk glass interface shown with a dashed line.

Dobkowice

An SEM-BSE image of a polished section of a glass bead from the Dobkowice burial site is shown in Fig. 10A. Surficial alteration of this sample takes the form of a distinct thin layer surrounding the entire sample. The layer appears to exhibit spalling, which is most likely an artifact created during sample embedding in epoxy. The actual boundary of the spalling is not strictly correlated to the boundary of the alteration layer with the bulk glass. The high-resolution SEM-BSE image in Fig. 10B shows that the layer is composed of a relatively homogenous ~50 µm-thick surficial layer (SL#1) having a sharp interface with the bulk glass. There is also a very thin and heterogenous over-layer (SL#2) that represents the topmost part of the alteration layer; note that these two layers resemble those in Fig. 8. The SEM-EDS map in Fig. 10C shows that the surficial layer can have variable thicknesses, here it is on the order of 50–100 µm. The principal alteration layer (SL#1) is depleted in Na, enriched in Si, and displays a more complex morphology, as evidenced, for example, by the Al-rich vesicle (this vesicle is further highlighted in Supplementary Fig. 1, which shows individual SEM-EDS maps of Fig. 10C). It is unclear if the Al-rich vesicle is the result of a glass alteration process or if it is soil that was incorporated into the surficial layer. This vesicle bears an uncanny resemblance to vesicles seen in oceanic basalt glasses that have been ascribed as being due to microbially-enhanced dissolution95. Supplementary Fig. 2 shows SEM-EDS maps overlaid on SEM-BSE images from a non-polished “as-is” fractured surface from the Dobkowice sample, confirming that SL#1is Na-poor, Si-rich and is attached to the bulk glass, thereby confirming that the spalling in Fig. 10 is due to sample preparation.

Fig. 10: Analysis of bulk glass and surficial layer for a glass bead from the Dobkowice burial site.
figure 10

A SEM-BSE image of Dobkowice sample in cross-section. B SEM-BSE image showing two surficial layers (SL#1 and #2) that formed during alteration. C SEM-EDS map overlaid on SEM-BSE image showing complex microstructure in one portion of the surficial layer SL#1. The small Al-rich growths are considered equivalent to SL#2.

The SEM-BSE and ToF-SIMS images in Fig. 11 reveal that in this portion of the Dobkowice sample, there exists a dominant alteration layer (SL#1) with a uniform thickness of approximately 50 µm. There is very little mass-density difference between SL#1 and the bulk glass. The large crack is an epoxy-embedding artifact and should not be confused with the SL#1 interface with the bulk glass. The ToF-SIMS chemical maps in Fig. 11 illustrate that the principal layer (SL#1) is hydrated (as shown in the H map), enriched in Si, Ca, and just slightly in Mg, and depleted in Na and K. The principal alteration layer has a very thin external rim (SL#2) characterized by strong Al and K enrichment as previously observed by other researchers64.

Fig. 11: SEM-BSE image and corresponding ToF-SIMS maps of the Dobkowice sample.
figure 11

The chemical maps show that the principal alteration layer (SL#1) is enriched in H, Si, Ca, and just slightly in Mg, whereas Na and K are depleted. Arrows demarcate the SL#1-bulk glass interface. The thin outer rim (SL#2) is enriched in Al and K. The prominent crack is an artefact.

Broborg

Sample BB1b was originally excavated from the Broborg hillfort, as described in the literature16,36,96,97. It was selected for study because it has a significant fraction of glassy material, and the surface appeared altered through natural processes96,98. Figure 12 shows an optical microscopy image and SEM-EDS elemental maps of the sample prepared in cross-section (individual maps shown in Fig. S3). In Fig. 12, the term ‘bulk’ refers to a glassy phase that was created during the melting of the protolith rocks and ‘SL’ refers to the surficial layer. The surface of the bulk glass is predominantly mafic, as the mafic glass is two orders of magnitude less viscous than the felsic glass, and therefore very likely flowed over the felsic material98. Compared to the bulk mafic glass, the surficial layer shown in Fig. 12B is enriched in Si and depleted in Na, Al, Mg, Ca, and Fe. The surficial layer in Fig. 12C is also depleted in Na and Fe, and enriched in Si. Ca is depleted, except for certain hotspots with elevated concentrations. The behavior of Mg and Al in the surficial layer is more complex, with areas of both enrichment and depletion. The textural and chemical heterogeneity of the bulk glass makes the evaluation of surficial layer formation challenging in samples from the Broborg hillfort.

Fig. 12: Optical microscopy and SEM-EDS elemental maps of Broborg sample BB1b in crosssection.
figure 12

A Optical microscopy image of Broborg sample BB1b with red arrows showing the location mapped by SEM-EDS. B, C SEM-EDS elemental maps overlaid on SEM-BSE. SL surficial layer.

SEM-EDS maps of a larger area of the Broborg BB1b sample are shown in Fig. 13, highlighting the surficial layers associated with the mafic region (individual maps shown in Fig. S4). The alteration layer is highly irregular in morphology and has an approximate average thickness of 13 µm. Some of this morphology may have a biological origin (e.g., see oval object on the left side of SL). The chemical composition of the altered layer differs from the amorphous matrix: Si is enriched, Al is depleted, and Fe, Mg, and Na are completely absent, having concentrations below the detection limit (see individual SEM-EDS elemental maps in Fig. S4). Figure 13 shows the textural and chemical heterogeneity of the bulk glass with feldspar needles, and irregularly shaped iron-bearing pyroxenes and spinels (identified by X-ray diffraction in Matthews et al.96) that are present throughout the glassy matrix. These crystalline phases are also present at the interface to such an extent that the glass matrix is rarely in contact with the surficial layer. The aqueous alteration rates of crystalline silicates and spinels are predicted to be significantly slower than silicate glasses. It is uncertain whether alteration of the glass proceeded until the alteration front reached a crystallite, or if these phases crystallized near the surface of the original bulk glass. However, it can be hypothesized that the composition and structure of the underlying matrix had a direct impact on the surficial altered layer.

Fig. 13: SEM-EDS maps of Broborg sample BB1b showing a surficial layer (SL) that formed in contact with the mafic glass.
figure 13

The arrows indicate the interface between bulk glass and the SL.

Newberry

Results are presented for three samples (MJS-1, BOF-6, and BOF-9) from the Newberry volcano Big Obsidian Flow. Samples BOF-6 and BOF-9 were both excavated in the same approximate vicinity; however, BOF-6 was partially covered in soil, while the BOF-9 sample was excavated from one of the walls of the obsidian flow. Sample MJS-1 was taken from the top of the flow. Figure 14 shows optical microscope and SEM-BSE images of the studied obsidian samples, including photographs taken from near the excavation sites of the three Newberry samples. Visually, the surfaces of MJS-1 and BOF-6 (Fig. 14A, E, respectively) both appeared white, while the surface of BOF-9 had a reddish tint (Fig. 14C). However, the BOF-6 surface was much more friable, while the surface of MJS-1 was consolidated. Both the MJS-1 and BOF-6 samples contained evidence of plant roots present on their surfaces.

Fig. 14: Optical microscopy and SEM-EDS elemental maps of obsidian samples from Newberry.
figure 14

A, C, E Photographs of Newberry obsidian outcrops and samples MJS-1, BOF-9, and BOF-6. B, D, F Corresponding cross-sectional SEM-EDS elemental maps of the surface regions and underlying matrix (individual EDS maps are provided in Figs. S5S7).

The SEM-EDS elemental maps of sample MJS-1, in Fig. 14B, show a surficial layer that is relatively non-porous at this magnification and has a variable thickness, ranging from a few µm to ~15 µm, with an average of 9 µm. The SEM-EDS chemical map of the BOF-9 sample in Fig. 14D shows that the red-colored surficial layer is composed of a highly porous, sponge-like structure that is compositionally similar to the underlying obsidian glass, with a minor fraction of particles being either Fe or Na-rich. The SEM-EDS chemical map of the BOF-6 sample, shown in Fig. 14F, reveals a smooth surface that is amply covered with silicon-rich features that are most likely diatoms99. At the scale of the analyses, there is no obvious evidence of an altered layer of significant thickness. Single element SEM-EDS maps of MJS-1, BOF-6, and BOF-9 can be found in Figs. S5S7, respectively.

Figure 15 shows ToF-SIMS ion maps of the altered layer of sample MJS-1. The maps show a ~10 µm-thick surficial layer with sharp chemical boundaries at both the inner and outer interfaces. The altered layer appears to be very heterogeneous with respect to its structure and composition, as shown in the SEM-BSE image (Fig. 15). This heterogeneity is also reflected in the chemical maps, which often show localized regions of enrichment and depletion. Na and K are generally depleted in this layer, while H, Mg, Al, Si, Ca, and Fe are enriched locally. The depleted and enriched layers are spatially coincident for all elements. The one exception is H, as this element displays two zones: (1) a prominent outer zone of elevated H enrichment ~10 µm thick; and (2) an adjacent, inner zone ~4 µm thick that is characterized by H concentrations just barely above that of the bulk obsidian. Both H zones have relatively sharp boundaries at the scale of the image. This contrasts with the H map of the Timna sample (Fig. 8), which showed only one layer of H enrichment with sharp interfaces.

Fig. 15
figure 15

SEM-BSE image and ToF-SIMS maps of Newberry obsidian sample, MJS-1.

Discussion

The natural and archeological analogs presented here were exposed to different environments for different lengths of time. The analogs were of different chemistry, a parameter that is intimately tied to technological developments, including the ability to melt materials at increasingly higher temperatures due to improvements in the high-temperature processing technologies that were employed, as well as the chemistry of the primary material sources used (important for controlling such factors as chemical impurities and oxidation state100). The factors of environment, length of time, and chemical composition of the starting material had an influence on the chemistry and morphology of the surface layers and secondary phases that developed in contact with the unaltered bulk glasses. These factors are summarized along with average altered layer thicknesses in Table 4. The use of altered layer thicknesses to compare and estimate rates of glass corrosion should be viewed as very approximate for many reasons. One reason is molar volume changes between the unaltered glass and the phase(s) making up the altered layer. Moreover, the effects of porosity in the altered layer also must be considered. It also cannot be excluded that over time, during burial and then retrieval from the soil, some of the surface altered layers may have lost their structural integrity, causing secondary phases to peel or break off, thereby making the altered layers incomplete and thinner.

Table 4 Summary of analog glass site data

The archeological samples described in this study were excavated from near-surface conditions in hydraulically unsaturated environments. This is important as the information garnered from the studied samples can be used to support the disposal of LAW glass at the Hanford site IDF. The nominal conditions at the Hanford IDF are an average subterranean temperature of 15 °C at 7.6-m depth, with an annual rainfall of ~180 mm101. After the waste and associated backfill have been placed in the facility, it will be covered with an engineered surface barrier. An infiltration rate of 0.5 mm/year is assumed while this barrier is intact, with the infiltration rate increasing to 3.5 mm/year once the barrier has degraded (after ~500 years)101. Water infiltrating through the backfill will chemically react with the dominant minerals present, which are mostly comprised of silica, as well as some carbonates. The carbonates minerals will lead to buffering of the pore water to neutral-to-mildly alkaline pH conditions. The IDF temperatures and annual rainfall quantities are closer to those of Timna than the other analog sites. The glass compositions expected at the IDF are different from the glasses from the analog sites, having lower Si, Fe, and Al, higher Na, as well as components that are not present in the analogs, including B, Li, V, and Sn. The Ballidon site and other field-testing sites will provide important data on the alteration of compositionally relevant borosilicate glasses in near-surface conditions relevant to the Hanford IDF. Analysis of alteration observed on archeological and modern glasses (including one borosilicate composition) buried at the Ballidon site for 52 years is described in Thorpe et al.76. Furthermore, analysis of US and UK nuclear waste type glasses buried for 18 and 20 years, respectively, is underway and includes borosilicate, silicate, and Fe-phosphate compositions. An additional test with buried LAW glass samples has also been underway since 2019, and data from those tests will be relevant to glass behavior in the IDF86, even though the duration of those tests is much less than that achievable with the archeological glass samples.

The present work characterizes the surficial alteration features of natural and archeological glasses as a function of the burial environment and the bulk glass composition. The characterizations that were performed confirmed that the samples contained a significant fraction of glassy material. These glassy materials were subjected to alteration under near-surface conditions for periods exceeding 1000 years and fulfill the criteria to be considered as an alteration analog, since they4,6,102: (1) are of a known or determinable chemistry (e.g., composition and structure); (2) are from a known or determinable alteration environment (e.g., exposure time, biological contact, solution chemistry, etc.); (3) are of a known or determinable provenance following its excavation (e.g., storage conditions, sampling history, conservation/restoration, etc.); and (4) are measurably altered. The physico-chemical characterizations revealed that differences in the chemical composition of the original samples significantly affected their chemical durability. The data in Table 4 suggest that the average annual air temperature and annual precipitation also have a measurable effect on the observed thickness of the altered surficial layer. Due to the nature of the analogs and their environments (lack of duplicates, different compositions, different temperatures, different rainfall, etc.), it is challenging to isolate the parameter that has the greatest effect on surficial layer thickness, and further characterization of samples from additional sites is needed in the future. However, the data show that samples altered in the arid Timna environment have thinner surface layers than samples subjected to greater annual precipitation levels.

It is important to note that air temperature and average precipitation do not fully parameterize the exposure conditions for these samples, and that future work will investigate the influence of the soil pore water chemistry and the local microbial community on glass alteration. During efforts to characterize and assess the Broborg glasses as alteration analogs, evidence of microbial interaction with the glass surfaces was observed via SEM19. Further microscopic and spectroscopic analyses showed glass alteration (chemical and morphological) consistent with microbial activity, evidenced by surficial pitting beneath microbes, suggesting a microbial component to glass corrosion103. Bacterial and fungal communities can colonize a variety of natural and synthetic materials, including rock and glass, by forming complex biofilms on the surfaces33. These microbial biofilms are known to weather these material surfaces using biophysical and biochemical processes (such as penetrating within cracks, producing extracellular polysaccharides, and secreting organic acids)104. Decades of research have established that microbial communities can persist and even thrive in harsh and toxic environments, suggesting the potential for biotic processes to influence the alteration of vitrified low-level nuclear waste after storage in near-surface geological facilities33,103,105,106. However, most studies evaluating the long-term durability of vitrified nuclear waste glass have focused on the abiotic degradation of these materials in sterile environments104. While the presence of microbes in these geological facilities is recognized107,108, only a few studies have attempted to characterize and extrapolate the observed short-term microbial impacts to predict the long-term (i.e., thousands of years) bio-alteration of vitrified nuclear waste, and this is therefore an ongoing area of research33,104,109,110.

To conclude, the knowledge obtained on how different environmental factors influence the alteration of vitrified archeological samples can be applied to vitrified nuclear waste materials. The subsequent incorporation of these factors into performance assessment models will allow for the development of a more holistic long-term prediction of the vitrified material durability under field conditions.

Methods

One of the main goals of the present study is to provide a general physical and chemical characterization of altered glass analogs recovered from the five sites. The techniques used provide information at various scales, with a maximum of micrometer-spatial resolution. Future work will involve techniques that have much higher spatial and mass resolution, such as transmission electron microscopy (TEM), atom probe tomography (APT), TEM-tomography, nano secondary ion mass spectrometry (nanoSIMS), etc., to better characterize the altered samples. Such high-resolution analysis techniques have been shown to provide significant insights into the interfacial region that delimits the boundary between the non-altered parent material and overlying authigenic surface layers (SL). Atomic scale measurements are crucial for future interpretations of the mechanisms of alteration95,111,112,113.

Optical microscopy, scanning electron microscopy (SEM), and electron probe microanalysis (EPMA)

Optical microscopy was performed with a Keyence VHX 7000 optical microscope. Samples were observed either ‘as received’, to evaluate surficial layers prior to any additional sample preparation involving exposure to water, or processing for polished sections for detailed characterization of the chemistry and morphology. Polished sections were made by first fracturing bulk material, embedding grains in epoxy, and then polishing sequentially with 240, 320, 400, 600, 800, and 1200 grit SiC abrasive paper in the presence of water (exposure to water during polishing is on the order of minutes compared to the hundreds of years the archeological samples have been in contact with water). The very limited exposure to water should have a negligible impact on alteration layer thickness and morphology). This was followed by polishing with a 1-μm diamond paste suspension.

Much higher spatial resolution imaging of polished sections was performed using a JEOL 7001 F SEM operated with a 15 kV accelerating voltage and 13 nA probe current. Energy-dispersive spectroscopy (EDS) analyses were performed with a Bruker Xflash 6 60 X-ray detector with a spectral resolution of 129 eV. Energy-dispersive X-ray spectra were processed using Bruker Esprit v2.1 software. Higher accuracy chemical composition measurements were made by electron probe microanalysis (EPMA) using a JEOL 8530 instrument operated with a 15 kV accelerating voltage and 20 nA probe current. Wavelength-dispersive spectroscopic (WDS) measurements were made with five spectrometers for high-energy resolution compositional measurements and analysis of light elements.

X-ray computed tomography

The internal 3-D microstructure of the samples was analyzed using X-ray micro-computed tomography (micro-CT) using a Thermo Fisher Scientific Heliscan Micro-CT system. Samples were mounted on styrofoam and scanned with an 80 kV p unfiltered microfocus X-ray source with a <1.5 µm diameter focal spot. Projections were acquired in a space-filling trajectory with a detector shift applied to help lessen the impact of pixel-specific artifacts. The acquired projections were reconstructed on a GPU cluster using iterative methods, yielding digital 3D volumes with voxel sizes around 5 µm3. Image segmentation was performed on the X-ray projections to partition the projections into: (1) bulk phase of the samples (assumed to be the amorphous phase); (2) bright inclusions (assumed to be crystals); (3) voids; and (4) background. The segmented projects were then stitched together to form a reconstructed 3-dimensional representation of the samples. The voxels corresponding to the amorphous phase were summed and normalized to the total volume of the amorphous and crystalline phases.

X-ray diffraction (XRD)

XRD was performed with a Bruker Advance D8 X-ray diffractometer using a Cu Kα X-ray source operated at 40 kV and 40 mA. Samples were either in bulk form or fine powders produced using a tungsten carbide mill. For semi-quantitative amorphous fraction analysis, sample powders were mixed with a 5 wt.% CeO2 internal standard. XRD scans were collected from 5–70° 2θ with a step size of 0.015° and a dwell time of 30 s. Phase identification of XRD patterns was carried out with EVA 4.0 using the PDF4+ database from the Inorganic Crystal Structure Database (ICSD). Rietveld refinement was used for semi-quantitative analyses of the amorphous sample fractions with TOPAS 4.0 software.

Time of flight secondary ion mass spectroscopy (ToF-SIMS)

ToF-SIMS measurements were performed using a ToF.SIMS5 instrument (IONTOF GmbH, Münster, Germany). ToF-SIMS has many advantages over SEM-EDS, including improved elemental detection limits and the ability to measure hydrogen (H). The distribution of H in the alteration layer of polished analog samples was measured using experimental conditions optimized for high signal-to-noise (S/N) ratios of H114. A 25.0 keV Bi+ beam was used as the analysis beam to collect positive secondary ion maps of the following ions: H+, Li+, Na+, Ca++, Ca+, 30Si+, Si+, Al+, Mg+, C+, K+, Cu+, and 54Fe+. A 1.0 keV O2+ sputter beam with 240 nA current was used before and during analysis to remove surface contamination and control the hydrogen background. The O2+ beam was scanned over a 700 × 700 µm2 area for 600 s before data collection to remove surface contamination. During the collection of ion maps, the instrument was operated in a non-interlaced mode. The Bi+ beam was focused to a 400 nm diameter with a beam current of 1.70 pA at 20 kHz frequency. Maps were acquired over 200 × 200 µm2, 150 × 150 µm2, or 50 × 50 µm2 areas with 256 × 256 pixels. During non-interlaced mode imaging collection, each cycle was composed of three steps: (1) the O2+ beam was scanned over the sample for 1 s to remove H adsorbed on the surface to control the H background, (2) a 0.5 s pulse was used for charging control so that reasonable signal intensity could be achieved, (3) 2 scans for ion map collection, with 256 × 256 pixels per scan. A total of 50–200 scan cycles were accumulated during data collection.

Chemical digestion and aqueous elemental analyses

Chemical digestion was carried out by microwave-assisted acid digestion. Inductively coupled plasma-optical emission spectroscopy (ICP-OES) analysis was performed on an Agilent 5110 VDV (Agilent Technologies, Santa Clara, CA) for major elements. Inductively coupled plasma-mass spectrometry (ICP-MS) was performed with a Perkin Elmer model NexION 2000B for trace elements (i.e., Cr and Zr). The chemical digestion procedure and subsequent elemental analyses were performed following test protocol USEPA3052B115.