The sequestration of metal ions into the crystal structure of minerals is common in nature. To date, the incorporation of technetium(IV) into iron minerals has been studied predominantly for systems under carefully controlled anaerobic conditions. Mechanisms of the transformation of iron phases leading to incorporation of technetium(IV) under aerobic conditions remain poorly understood. Here we investigate granular metallic iron for reductive sequestration of technetium(VII) at elevated concentrations under ambient conditions. We report the retarded transformation of ferrihydrite to magnetite in the presence of technetium. We observe that quantitative reduction of pertechnetate with a fraction of technetium(IV) structurally incorporated into non-stoichiometric magnetite benefits from concomitant zero valent iron oxidative transformation. An in-depth profile of iron oxide reveals clusters of the incorporated technetium(IV), which account for 32% of the total retained technetium estimated via X-ray absorption and X-ray photoelectron spectroscopies. This corresponds to 1.86 wt.% technetium in magnetite, providing the experimental evidence to theoretical postulations on thermodynamically stable technetium(IV) being incorporated into magnetite under spontaneous aerobic redox conditions.
Natural minerals can host, or incorporate into their crystal structure, different elements and function as sinks attenuating environmental transport of heavy metals and radionuclides. Garnet, gypsum, calcite, muscovite, rutile and other mineral phases are found to contain incorporated Tc, Ru, Cs, U, Np, and Pu1. Iron minerals, such as iron oxides (magnetite, maghemite, and hematite), and iron oxyhydroxides (goethite, lepidocrocite, ferrihydrite, etc.) also incorporate various metal cations, in particular, substitution of Fe3+ by Al3+ can reach up to 33 mol.% in natural weathered goethite and up to 15 mol.% in maghemite in tropical soils2. Computational studies on Tc4+ incorporation in magnetite revealed thermodynamic feasibility to obtain up to 5 wt.% of incorporated Tc4+ with higher stability around 1–3 wt.%3, however, no experimental studies were carried out to support the upper limit of Tc incorporation in the ambient uncontrolled environment. Further, formation of iron minerals is complex as it yields an array of transformation pathways for different stable oxides/oxyhydroxides2. This allows for design of plentiful systems targeting a specific mineral formation in which an element of interest is being incorporated. Particularly, there is practical significance to employ widely available metallic iron (Fe0), encouraging investigation of its oxidative transformation with the possibility of concomitant sequestration of radionuclides undergoing simultaneous reduction, e.g., Tc, in a system under ambient conditions where only a limited number of controlled parameters are imposed to resemble natural pathways.
The radioisotope of technetium, 99Tc, is a β− emitter of predominantly anthropogenic origin that generates environmental risk in sites impacted by cold war era development of nuclear weapons (e.g., Hanford site WA, USA;4 Mayak, Russia5) or nuclear accidents (e.g., Chernobyl, Ukraine6), and its environmental impact is amplified by a long half-life (213,000 years) and redox-dependent mobility with high solubility of the pertechnetate anion (TcO4−) in aerobic conditions7. Under anoxic conditions Tc reductively precipitates as hydrous TcO2 and can be retained in iron-rich sediments even upon consequent exposure to air8. The possibility of utilizing iron-based phases as reductive separation and sequestration agents initiated numerous studies on Tc immobilization into iron minerals9,10,11,12,13,14,15,16,17,18,19. The majority of these studies investigated reductive removal of Tc from solution via structural incorporation into in situ formed mineral iron oxide/oxyhydroxite phases, i.e., ferrihydrite, magnetite, hematite, and goethite, starting with soluble homogeneous Fe2+ precursors20. Immobilization of Tc within the crystalline structure of a host helps to achieve recalcitrant oxidative leaching of Tc4+, and synthesized Tc4+-doped magnetite, hematite and goethite that have been evaluated as durable waste forms for long-term geological disposal demonstrated relatively low Tc release rates13,14,21. When structurally incorporated into in situ formed magnetite, Tc4+ was prone to remain in the reduced state even upon oxidation of magnetite15. Tc4+-doped magnetite (Tc0.06Fe2.94O4) can be synthesized with 2.5 wt.% Tc by dissolving a small amount of iron powder in a denitrated solution of Tc21, however, incorporation of Tc4+ into pre-synthesized magnetite was found to be sensitive to its initial concentration16. Although in situ formed magnetite was more efficient for Tc reductive sequestration than the pre-synthesized one, these studies have been conducted in anoxic conditions. Iron oxidation in anoxic vs. oxic conditions would take a different route with water or dissolved oxygen serving as an oxidant, leading to dissimilar iron oxidation pathways2.
There are limitations of utility of the homogeneous in situ synthesis of iron minerals for the practical separation systems design when it utilizes prone-to-oxidation Fe2+, as it must be carried out in a controlled pH and redox sensitive environment, and therefore can’t be accomplished in complex aqueous matrices directly, necessitating prior separation of Tc from the original host streams. A valuable alternative is in situ mineral transformation of a metallic iron, Fe0, or zero valent iron (ZVI), potentially offering continuum reductive separation and structural incorporation of Tc under ambient conditions from complex aqueous electrolyte mixtures over wide pH and concentration ranges, albeit via poorly understood mechanisms. Overall, ZVI is a readily available strong reductant that has been proposed for decontamination and remediation strategies, including reductive removal of radioactive contaminants, uranyl and pertechnetate, in groundwater22,23,24. ZVI (iron powder, nano-iron, and steel coupons) exhibits effective reductive separation of Tc25,26,27, and is one of the materials compatible with immobilization and stabilization of the separated Tc for long-term disposal, but its application can be modulated by Tc anticorrosive properties28,29, and has not been investigated for high Tc loading. Different iron oxides/oxyhydroxides can be formed during reaction of metallic iron in aerobic conditions, and their transformation pathways are influenced by a variety of factors, including presence of anions2, where effect of TcO4− at moderately high concentration has not been studied yet. In addition, ZVI materials have shown different redox kinetics, depending on particle size and related to their manufacturing method27. Thus, the behavior of an iron system requires additional investigation for each unique setting and contaminant of concern.
Here, we seek a fundamental understanding of the in situ formation of iron oxide phases in the aerobic environment governed by the redox equilibria processes. We study a heterogeneous oxic system containing solid Fe0 and aqueous TcO4− initiating surface redox reactions associated with Fe0 dissolution, followed by in situ co-precipitation with Tc4+ reduction products. Our previous testing of a wide range of commercial iron products27 shows that granular ZVI exhibits 99% Tc-removal efficiency indicating kinetics suitable for time-dependent structural studies on formation and transformation of iron minerals in the presence of Tc. The NaCl solution matrix is chosen in order to supply an electrolyte that promotes iron oxidation2 and avoids complexation with TcO4−, i.e., without interfering with the Tc7+ reduction process30. All experiments of reductive sequestration of Tc with granular ZVI and comprehensive characterization of solid phases are conducted at Fe:Tc molar ratio 53:1, or 3.3 wt.% Tc. The results show structural incorporation of Tc4+ at the high loading and reveal effect of Tc on transformation of iron mineral phases.
Reductive removal of pertechnetate
After 25 days of contact time of granular ZVI with 80 mM NaCl solution containing 17 mM TcO4−, 99.8% of the aqueous Tc was removed from the solution (aqueous fraction of Tc 0.0010 ± 0.0004). In the presence of Tc, ZVI granules exhibited distinct time-dependent changes observable by color (Supplementary Fig. 1a, b), transitioning from brown-yellowish after a week to smaller black granules after a month from the start of the experiment. In the absence of Tc, the sample of ZVI reacted with 80 mM NaCl solution turned black within one week after the start of the experiment (Supplementary Fig. 1c). Both samples with and without Tc had a fraction of newly formed black suspended fines (likely magnetite), separated during several runs of consecutive centrifugation, and analyzed as a bulk solid phase with the rest of solids per each sample. The concentration of Tc in the supernatant was 0.01 mM of TcO4−. After centrifugation, samples were washed with deionized water, and the washing solution had slightly higher Tc concentration (0.08 mM) compared to the supernatant. This suggested possible re-oxidation or resuspension of Tc4+.
As investigated previously, ZVI materials manufactured by different methods exhibit different kinetics of Tc removal, attributed to variable surface properties and rates of Fe0 oxidation and dissolution27. Among the wide variety of ZVI materials tested previously, granular iron belonged to a group with superior Tc7+ reduction efficiency, and it exhibited the least propensity for Tc4+ re-oxidation within this group. For this material, the profile of Fe0 solubilization in 80 mM NaCl solution and the corresponding pH and ORP time dependencies had been studied earlier27. Here, the pH value of 10.3 measured 25 days after the start of experiment indicated the prevalence of iron dissolution reactions2.
X-ray absorption near edge structure (XANES) analysis from different locations (A and B) on two iron granules (ZVI-1 and ZVI-2) showed that both Tc4+ and Tc7+ were present in the solid phase after one month of contact with ZVI (Table 1); however, partial oxidation of Tc4+ during sample preparation, storage, and analysis cannot be ruled out. Linear combination fitting (LCF) was performed for XANES (21 to 21.4 keV) and extended X-ray absorption fine structure (EXAFS) spectra (3 < k < 12), and LCF combinatorics showed better statistical results for three components, with R-factor and Chir2 almost two times smaller for three components vs. two components (Supplementary Table 1). Moreover, principal component analysis (PCA) was supportive of three components (Supplementary Fig. 2); hence, three standards were kept for LCF (Fig. 1a; Table 1), two of which were Tc4+ with different coordination environments (Tc4+ hydrated oxide and Tc4+ in magnetite). These results revealed that approximately 50% of Tc was present as TcO2•nH2O in addition to 34% of Tc in Tc4+ phases associated with iron oxides. The remaining small fraction of Tc was associated with adsorbed Tc7+ phases with a larger fraction present in B locations of both granules, where more Tc was associated with the solid phase, as seen from the false-color abundance maps, Fig. 1b (11–13% in A locations vs. 20–21% in B locations, Table 1).
We further performed high-resolution X-ray photoelectron spectroscopy (XPS) analysis of the ZVI granules (Fig. 2). Peak fitting of the Tc 3d spectrum required three pairs of doublets, whose lower binding energies (3d5/2) were determined to be 256.4 eV, 257.4 eV, and 259.6 eV. While the peaks at 256.4 eV and 259.6 eV were assigned to Tc4+ (35.3%) and Tc7+ (32.8%), respectively31,32, the peak at 257.4 eV suggested Tc4+ in a different local environment (~31.9%) that is supported by XANES analysis (Fig. 1a and Table 1).
Structural characterization of solid phase
Powder X-ray diffraction (PXRD) analysis of ZVI granules contacted with 80 mM NaCl solution with and without TcO4− was indicative of magnetite in all samples, with a more prominent magnetite pattern in samples without Tc, Fig. 3ab (data with Rietveld refinement are in Supplementary Fig. 3). Here, PXRD patterns did not allow for the discrimination between magnetite and maghemite, hence, maghemite formation was not excluded. In addition, the single crystal diffractogram of the one-month contacted ZVI sample without Tc revealed an additional iron phase, ferrihydrite (Supplementary Fig. 4); the sample with Tc did not produce a good signal.
XPS core level Fe 2p spectrum (Supplementary Fig. 5) showed a profile characteristic of Fe3+ 33,34, with an Fe 2p3/2 peak at 711.2 eV and a signature satellite peak at ~719 eV, which may belong to maghemite. It should be noted that XPS is a surface sensitive technique with a sampling depth of <10 nm, and oxidized surface layers, i.e., magnetite oxidized to maghemite, may not be representative of the bulk.
Mössbauer spectroscopy confirmed the presence of non-stoichiometric, or partially oxidized, magnetite. Magnetite (Fe3O4) is an inverse spinel which has stoichiometry of 8 tetrahedral Fe3+, 8 octahedral Fe3+, 8 octahedral Fe2+, and 32 O atoms with Fe2+/Fe3+ ratio equal to 0.5. Oxidation of magnetite leads to formation of maghemite (γ-Fe2O3) with a unit cell of 8 tetrahedral Fe3+, 13 1/3 octahedral Fe3+, 32 O atoms, and 2 1/3 vacancies for charge balance at octahedral sites, and its stoichiometric Fe2+/Fe3+ ratio is 0 at complete oxidation of magnetite. The experimental Fe2+/Fe3+ stoichiometry can be determined using Mössbauer signals as Fe2+/Fe3+ = 0.5 octFe2.5+/ (0.5 octFe2.5+ + oct,tetFe3+), where oct,tetFe3+ is an overlapped sextet signal from tetFe3+ and octFe3+ in partially oxidized samples, and octFe2.5+ is a sextet of octahedrally coordinated Fe2+ and Fe3+35.
Two sextets of octahedral-tetrahedral Fe3+ and octahedral Fe2.5+ were well-distinguished in the room temperature Mössbauer spectra of ZVI samples not exposed to Tc (sample oxidized for one week: Supplementary Fig. 6a; and sample oxidized for one month: Fig. 4a). Longer contact time led to partial oxidation of magnetite (Fe2+/Fe3+ < 0.50), as the Fe2+/Fe3+ ratio decreased from 0.47 (one week contact time) to 0.39 (one month contact time), suggesting an effect of the topotactic transformation of magnetite, i.e., maghematization process2. A time-dependent increase of the magnetite-maghemite content in the samples without Tc was accompanied by the expected decrease of the Fe0 phase (Supplementary Table 2).
Room temperature Mössbauer spectra of the ZVI samples contacted with Tc for one week and one month were both dominated by Fe3+ doublets at 0–0.78 mm/s (Supplementary Fig. 6b) and at 0–0.72 mm/s (Supplementary Fig. 6c), respectively, that could be attributed to a mixture of phases, such as nano-sized magnetite36, nano-sized maghemite37, lepidocrocite38, nano-sized goethite39, or ferrihydrite10. The PXRD analysis excluded the dominant presence of goethite and lepidocrocite (Fig. 3); ferrihydrite was not easily evident due to its poorly crystalline nature, but its presence was supported by the results from single crystal analysis for the ZVI sample without Tc (Supplementary Fig. 4). Liquid nitrogen Mössbauer spectroscopy measurements allow identification of nano-sized magnetite and poorly crystallized maghemite resolved as a sextet due to superparamagnetic relaxation36,37. For this purpose, additional spectra of the one-month aged sample were taken at 77 K and provided evidence of a Fe3+ doublet at 0–0.81 mm/s, comprising 27% of total iron and proving presence of ferrihydrite; the remaining spectral features were resolved as the sextets of octahedral-tetrahedral Fe3+ and octahedral Fe2+ (Fig. 4b). Decrease of the Fe3+ doublet area and increase of the Fe3+ and Fe2+ sextet areas relative to the room temperature measurements is attributed to the presence of nano-sized magnetite and/or maghemite. Another interesting observation is that the Fe2+/Fe3+ ratio in the room temperature spectrum was 0.33 compared to 0.39 for the analogous sample without Tc (Supplementary Table 2), which signifies a higher fraction of octahedral Fe2+ oxidized to Fe3+, hence, higher content of non-stoichiometric magnetite or magnetite-maghemite mixture in the sample with Tc. Distinction between non-stoichiometric magnetite and magnetite-maghemite mixture is known to be problematic40, and we further refer to it here as non-stoichiometric magnetite. The maghematization process is accompanied by the formation of vacancies during oxidation and loss of Fe2+. This process is energetically favorable for Tc4+ incorporation, where Tc4+ substitutes Fe2+ in the octahedral sites, and loss of two Fe2+ atoms satisfies the charge balance3. Moreover, as shown by Marshall et al.15, Tc4+ incorporated into magnetite is recalcitrant to oxidation and release during long-term transformation of magnetite to maghemite.
Furthermore, comparison of the Mössbauer spectra corresponding to the ZVI samples exposed to NaCl solution with and without Tc for one month revealed higher fractions of the unreacted Fe0 and Fe3+ (ferrihydrite) in presence of Tc (Supplementary Table 2; Supplementary Fig. 6). It should be noted that this analysis was primarily done for the purpose of qualitative assessment of the oxidized iron mineral phases.
Cubo-octahedral morphology pertinent to magnetite2,41 was observed by scanning electron microscopy (SEM) in the sample contacted with Tc for one month (Fig. 5). The surface of the iron oxide, formed as a result of ZVI dissolution and reprecipitation, was uniformly covered with Tc, as seen via energy dispersive X-ray spectroscopy (EDS) on particles contacted with Tc for one week (Supplementary Fig. 7) and on particles contacted with Tc for one month (Fig. 5). Moreover, Tc association with iron oxide (i.e., non-stoichiometric magnetite) was both on the surface and within iron oxide particles. Analysis of the lamella prepared by focused ion beam (FIB) showed that Tc was incorporated and homogeneously distributed well below the particle surface (Fig. 6). However, EDS performed at the nano scale revealed heterogeneous areas with local enrichment of Tc (Fig. 7).
High resolution scanning transmission electron microscopy (HR-STEM) analysis identified regions with the crystal structure consistent with maghemite or magnetite which cannot be distinguished because of close structural similarities (Fig. 7c). According to the Mössbauer spectroscopy results, the material in the images could be non-stoichiometric magnetite or a magnetite-maghemite mixture. In addition, EDS analysis of the edge of a particle revealed an area (approximately 100 × 200 nm) with little to no Tc present (Supplementary Fig. 8) which was also confirmed via HR-STEM to be either magnetite or maghemite. Further, HR-STEM analysis of the ZVI sample contacted for one month without Tc was consistent with the presence of magnetite or maghemite (Supplementary Fig. 9).
The presence of other iron mineral phases was not detected with STEM analysis, however the lamella did not represent the bulk sample (Supplementary Fig. 10). The amorphous powder-like solids were not suitable for FIB extraction, thus, additional iron mineral phases cannot be excluded. Scanning electron micrographs of ZVI samples with and without Tc showed larger particles in the sample without Tc, and more of the powder-like iron oxidation product (i.e., ferrihydrite) in the sample with Tc (Supplementary Fig. 11). Possibly, retarded transformation of ferrihydrite to magnetite resulted in smaller particles in the sample with Tc.
Extended X-ray absorption fine structure analysis
Extended X-ray absorption fine structure (EXAFS) data analysis and modeling were performed to clarify Tc4+ association with iron oxides (Fig. 8, Table 2). Even though non-stoichiometric magnetite or magnetite and maghemite mixture is referred to here, due to their structural similarities, a modified crystal structure of magnetite was used for the fitting model. The octahedral atom of iron (Fe1) was set as a core atom substituted by Tc. The coordination number (CN) of both octahedral Fe1 and tetrahedral Fe2 was fixed at 6.0 in accord with the crystal structure of magnetite. Theoretically, the first shell of octahedrally coordinated Tc4+ is represented by six O atoms in both oxide and magnetite. The majority of the EXAFS studies on Tc incorporation into magnetite fixed CN to 6.015,16,30,42, however, our data did not result in a good fit with 6O atoms, possibly due to a fraction of the Tc being on the surface of the iron oxide nanoparticles where its coordination numbers can be reduced. While the CN for ZVI-1-A and ZVI-2-A (4.4 and 4.1, respectively) are reasonable, accounting for the mixture of Tc7+ and Tc4+ and surface fraction of Tc4+, the CN for ZVI-1-B and ZVI-2-B are quite low (3.1 and 2.7, respectively), but the data for these scan locations correspond to the elevated amounts of Tc (false-color images with Tc abundance on ZVI granules, Fig. 1b), with a higher fraction of TcO4-, i.e., 0.21 and 0.20, respectively (Table 1), the contribution from which is not included in the fit. The path Tc—Tc (Table 2) implies the existence of Tc4+ oxide monomers and dimers11. Similar results were obtained for TcO2 sorbed to magnetite16, Tc4+ partially incorporated into magnetite18, and surface-precipitated TcO2•xH2O (not incorporated into goethite, or magnetite13) with the respective Tc—Tc atomic distances at 2.57, 2.56, and 2.51 Å and CN of 0.9, 1.2, and 0.5.
The obtained Tc-Fe1 and Tc-Fe2 atomic distances (Table 2) are in excellent agreement with the respective 3.12 and 3.52 Å reported by Yalçintaş et al.16. These distances are very similar to those reported in the studies on sorbed and incorporated Tc in magnetite13,15,18,30, implying an impossible differentiation of the paths between sorbed vs. incorporated Tc in the magnetite structure. Note that the large value of σ2 for the Tc-Fe1 path is an indication that the average CN of this path is lower, and is supportive of the heterogeneous system, where Tc has next-near neighboring Fe ions from the iron mineral, as well as Tc in a Tc4+ oxide. Moreover, distances between iron atoms in different iron minerals are very similar, and the EXAFS spectra of hematite, goethite, and ferrihydrite were found to be almost identical10,11. In such cases conclusive statements should not be made from EXAFS analysis alone, but in conjunction with other techniques20. As such, STEM and EDS results confirm association of Tc with iron oxide, i.e., non-stoichiometric magnetite, not only on the surface (Supplementary Fig. 6), but in the vertical profile of the lamella cut from the iron oxide with FIB technique (Figs. 6 and 7), showing a clustered Tc environment within the magnetite nanostructure. Possibly, the areas of local enrichment are mixtures of TcO2 monomers and dimers incorporated in the iron oxide’s crystal structure, where incorporation of mononuclear Tc4+ at the octahedral Fe site cannot be excluded. This is also supported by the XPS results, demonstrating two distinct environments for Tc4+. In addition, a model with contribution from the multiple scattering paths as an alternative to the iron shell scattering was tested and produced non-reportable results (Supplementary Table 3), supporting the evidence of incorporated Tc4+.
Oxidation of Fe0 in 80 mM NaCl in an aerobic environment resulted in near complete (99.8%) reductive removal of Tc7+ from solution after almost a month from the start of the experiment. The sample showed discernible differences in the fractional distribution of iron minerals in comparison with the specimen oxidized under the same conditions but without Tc. The fraction of ferrihydrite, four times larger in the sample with Tc, was accompanied with a smaller fraction of non-stoichiometric magnetite, and a higher content of non-reacted ZVI. We relate these observations to the slower transformation of ferrihydrite to magnetite in the presence of Tc.
Transformation of ferrihydrite, a hydrous ferric oxyhydroxide with a low degree of order, commonly yields hematite and goethite (ferric oxide α-Fe2O3 and oxyhydroxide α-FeOOH, respectively), where predominant formation of one or the other is strongly dependent on pH and temperature, as well as on the degree of ordering of ferrihydrite and presence of anions, cations, and neutral molecules2. Adsorption of foreign species or their structural incorporation into iron mineral phases suppresses transformation processes; with higher concentrations of divalent metal ions, ferrihydrite transforms into goethite, mixtures of hematite and spinel, or spinel only when molar fraction of divalent cation 0.33 and higher2,43. High concentrations of ferrous ions (Fe2+) induce a transformation path of ferrihydrite to magnetite (inverse spinel) at ambient temperature and pH >7 (faster at pH 9), which rapidly oxidizes to maghemite, as demonstrated in experiments with ferrihydrite and Fe2+ solutions41. In our study, the initial amount of iron in the sample is high (50 g/L), leading to high Fe2+ dissolution rates that are supported by pH 10.3 indicative of Fe0 oxidation/dissolution reactions2,27, implying that transformation of ferrihydrite to magnetite would prevail over hematite or goethite. The PXRD and Mössbauer spectral evidence reported here do not reveal a separate Fe2+ mineral phase, e.g., siderite or green rust, that could have been expected due to the presence of carbonate in aerated solution at elevated pH. Furthermore, microscopic analysis of the iron oxidation products (Fig. 5) is very similar to that reported for spinel formation in FeCl2 solution41.
As mentioned previously, the addition of foreign species, i.e., anions, in the system retards the transformation of ferrihydrite, and our observations relate pertechnetate to the category of such species. The magnetite fraction was noticeably suppressed in the samples of ZVI with Tc (Supplementary Table 2), resulting in slower transformation of ferrihydrite into magnetite, which was also supported by PXRD data, with the amount of magnetite comprising 2–7% in the Tc-loaded samples vs. amount of magnetite in the range of 15–26% in the samples without Tc (Supplementary Fig. 3). Moreover, in the presence of Tc, samples of ZVI granules did not oxidize as fast, as evidenced by the larger amount of Fe0 detected in the Tc-loaded samples via Mössbauer and PXRD analyses (Supplementary Table 2; Supplementary Fig. 3). These results are in accord with the fact that Tc is known for its anticorrosion properties28,29.
Our experiments, carried out with initial Fe to Tc molar ratio 53, or 3.3 wt.% Tc, indicated the feasibility of near complete reduction of Tc7+ (TcO4− determined via XANES analysis could be explained by surface oxidation during sample handling and/or exposure to the photon beam) with consequent incorporation of at least 32% Tc, as determined from XANES analysis (Table 1) and supported by XPS analysis, which identified ~32% Tc4+ in the local environment different from Tc4+ in the precipitated oxide (Fig. 2). This amount comprises an estimated 1.86 wt.% Tc in the magnetite (magnetite fraction was estimated via Mössbauer measurements of the one-month reacted sample). Interestingly, these results, corresponding to the thermodynamically spontaneous system, support theoretical calculations defining 5 wt.% as the energetically feasible, but unstable, upper limit for Tc incorporation into magnetite3 with increasing stability at 1.3 vs. 2.6 wt.% for Tc incorporation into hematite12. It is important to note that spinel ferrite with 4 wt.% Tc was synthesized by Lukens et al.17, however it pertains to a system under a controlled environment, i.e., TcO4− dissolved in Fe2+ solution followed by neutralization and heating. We emphasize the importance of a spontaneous system, analyzed here, as it relates to practical needs and may pave the way for remediation technologies and waste form development.
Further, our results showed heterogeneous distribution of Tc within the iron oxide (Fig. 7). Similar observations of clustered Tc in spinel ferrites have been reported previously for Tc0.1Fe2.9O417, and Tc4+ dimers were estimated to be the most stable clusters in doped rutile (TiO2)44. The study by Yalçintaş et al.16. reported Tc4+ dimers bonded to the surface of pre-synthesized magnetite at 0.2 mM Tc as opposed to partial incorporation of Tc4+ at 0.02 mM Tc (Fe:Tc molar ratios 1300–3200). It is known that substitution of magnetite is enhanced when the metal coprecipitates with ferrihydrite vs. when the metal is added after ferrihydrite precipitation2; that is why results for Tc incorporation are sensitive to relatively low Tc concentration of 0.2 mM16, when there is no in situ synthesis of iron oxides/oxyhydroxides. In contrast, we observed significant fractional incorporation of Tc4+ into iron oxide formed in situ during oxidation of Fe0 at elevated Tc loading, 17 mM TcO4− (Fe:Tc molar ratio 53). Such successful results can be explained by the compounded processes of Tc7+ reduction and ferrihydrite formation with further transformation to non-stoichiometric magnetite or magnetite and maghemite mixture during oxidation of ZVI.
99Tc emits β– radiation (0.29 MeV29). All radioactive samples were prepared at a nonreactor nuclear facility by certified and trained personnel inside of a fume hood designed for radiological contamination control.
The samples were prepared with granular ZVI (Alfa Aesar, electrolytic, 1–2 mm particle size, 99.98% purity) at a concentration of 50 g/L in 80 mM NaCl (Sigma Aldrich, ≥99.5%); neutral solution (pH 6.9–7.3) using double deionized water (DIW) of at least 18 MΩ·cm. A 99Tc stock, containing 40 g/L Tc as NH4TcO4, was used to prepare a working solution of 17 mM Tc in 80 mM NaCl which was added to granular ZVI samples (Fe to Tc molar ratio 53; or 3.3 wt.% Tc). All samples, with and without Tc, were placed on a shaking table for short-term (up to one week) and long-term (up to one month) contact times. Experiments were conducted at ambient temperature and pressure in the presence of air.
Concentrations of Tc7+ in aqueous phase were determined by a liquid scintillation counter (Tri-Carb 3100TR, PerkinElmer) after samples were centrifuged and aliquots of 10–50 µL of solution were mixed with 10 mL of a scintillation cocktail (Ultima Gold LLT, PerkinElmer). Results were background corrected and accounted for the 94% efficiency of the counter.
Solid phase characterization
All samples, with and without Tc, were centrifuged to separate solids and decant the liquid phase. Separated solids were rinsed with DIW, removed by centrifugation, and dried under nitrogen atmosphere to prevent oxidation. Samples were preserved under a blanket of nitrogen until analyses.
Powder X-ray diffraction (PXRD) data were collected for all samples using a Rigaku Ultima IV diffractometer equipped with a Cu sealed tube X-ray source, using a divergent slit of 1/2°, a height limiting slit of 10 mm, 5° Soller slits on the source and detector sides, a 2/3° scattering slit and a 0.15 mm receiving slit, a bent graphite secondary monochromator and a scintillation detector. The diffractometer goniometer radius was 285 nm. Each PXRD sample was prepared in a poly(methyl methacrylate) plastic sample holder with a 25 mm diameter by 1 mm deep sample well and a dome cap. PXRD data of one month contacted samples were collected by sticking a small quantity of powder to a MiTeGen MicroMount pin with silicon vacuum grease. The pin mounted powder was placed on a Bruker D8 Venture single crystal diffractometer equipped with a Mo Kα X-ray source monochromated with a bent germanium crystal and a 2-dimentional area detector. The sample pin was rotated axially (φ rotation) during data collection. Diffraction frame data was integrated using the EVA version 4 (Bruker) software in order to generate an intensity vs. 2θ angle plot. Data were collected also for NIST SRM 660c in order to determine the zero error and refine parameters by method described by Cheary and Coelho45 to account for instrument broadening. The diffraction data were analyzed using the TOPAS v6 software package. Identified phase components were quantified by the Rietveld method. Diffraction peak profile fitting was done using the double Voight method to account for peak broadening from crystallite size and micro-strain.
Mössbauer spectra were collected at room temperature for all samples, and, additionally, 77 K temperature analysis was used for the ZVI sample reacted with Tc for one month. The 50 mCi 57Co/Rh source and velocity transducer MVT-1000 (WissEL) operated in a mode of constant acceleration (23 Hz, ±12 mm/s). The signal was transmitted through a holder where radiation was detected by Ar-Kr proportional counter. The counts were stored in a multichannel scalar as a function of energy, utilizing a 1024-channel analyzer. Data were folded to 512 channels to give a flat background and a zero-velocity position corresponding to the center shift (CS or δ) of a metal Fe foil at room temperature. A 25-μm thick Fe foil (Amersham, England) was placed in the same position as the samples to obtain calibration spectra. The Mössbauer data were modeled using the Recoil software (University of Ottawa, Canada) and a Voigt-based structural fitting routine.
X-ray photoelectron spectroscopy (XPS) spectra were recorded on a Kratos AXIS Ultra DLD system equipped with a monochromatic Al Kα X-ray source (1486.7 eV) at 10 mA, 15 kV for excitation and a hemispherical analyzer. Data were corrected relative to the reference 285.0 eV carbon 1 s peak. The software CasaXPS (version 2.3) with Shirley type background and 20% Gaussian–Lorentzian ratio was used for peak fitting.
X-ray absorption near edge structure (XANES) and extended x-ray absorption fine structure (EXAFS) measurements of the Tc K-edge were obtained at the X-ray Science Division beamline 20-ID-C at the Advanced Photon Source (APS, Argonne National Laboratory). In addition, 2-D elemental maps were collected based on x-ray fluorescence mapping (XRM). Thin sections were prepared for the analysis. Dried solids were prepared in a 1.6 cm (ID) aluminum tubing with slow drying epoxy. Two parts of epoxy were mixed with one part of hardener (EpoThin2 epoxy and hardener, Buehler, Lake Bluff, IL) with a volume of 3 mL with 0.1–0.5 g of solids. Samples were then vacuum-degassed to remove bubbles and air-dried overnight at room temperature. Slices were cut with an Isomet 1000 diamond blade thin sectioning saw with Isocut fluid (Buehler, Lake Bluff, IL) to a thickness of approximately 150 µm. After mounting on a glass microscope slide, thin sections were sanded with silicon carbide sand paper with Isocut fluid followed by 400 grit sand paper, then 600 grit sand paper, and finally 1200 grit sand paper (Ted Pella, Inc.) all using a figure eight pattern. Final polishing was conducted with a Nylon polishing cloth and 1 µm diamond polish (Metadi II, Buehler). Samples were washed with methanol and dried prior to analysis. Samples of ZVI granules contacted with Tc were encased in epoxy resin and cut into thin sections. The sample was doubly encapsulated in mylar and Kapton films.
Spectra were collected in fluorescence mode using a 4 element Vortex (silicon drift) detector, Si 111 monochromator; Fe and Mo foils were utilized for energy calibration. Data were analyzed using ATHENA and ARTEMIS software (version 0.9.26)46. XANES spectra were analyzed via linear combination fitting with standards of Tc4+ in magnetite17, Tc4+ oxide47 and Tc7+ adsorbed onto Purolite A530E resin. ICSD files of Fe3O4 and TcO2 were used for FEFF6.0 calculations for fitting the EXAFS region; the magnetite input file was modified with a core Tc atom in an octahedral Fe site.
Scanning electron microscopy (SEM) images were obtained using a Quanta 250FEG SEM (Thermo-Fisher Inc., Hillsboro, OR) equipped with an EDAX Genesis™ (EDAX Inc., Mahwah, NJ) analytical energy dispersive X-ray spectroscopy (EDS) system. Scanning transmission electron microscopy (STEM) was performed on a cold field emission JEOL ARM 200 F operated at 200 kV and equipped with a Noran™ (Thermo Scientific, Waltham, MA) EDS system. The microscope is aberration-corrected with a hexapole-type probe Cs corrector (CESCORR, CEOS). STEM micrographs and EDS maps were collected with a 0.78-Å probe at an emission current of 15 µA, with a high-angle annular dark-field (HAADF) detector inner angle of 82.6 mrad. A lamella from the sample contacted with Tc for one month was prepared using a focus ion beam (FIB) on a Quanta SEM (Thermo Fisher FEI). The lamella was attached to a copper Omniprobe liftout grid using Pt welds. The sample aged without Tc produced loosely aggregated clumps of iron oxides and several lamellae from that sample fragmented before imaging. Therefore, the Tc-free sample was prepared for imaging by directly placing the dry particles onto a 200-mesh copper TEM grid coated with a holey carbon film (Electron Microscopy Supplies, Inc) and tapping off the excess.
Data supporting these findings are available within the article and supplementary information files.
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It is our pleasure to acknowledge help of C. T. Resch, S. Chatterjee, M. Fujimoto, W. W. Lukens, C. I. Pearce, K. Kruska, M. J. Olszta, R. G. Surbella, and D. L. Brewe. This research was supported by the U.S. Department of Energy’s Office of Environmental Management and performed as part of the Technetium Management Hanford Site project at the Pacific Northwest National Laboratory (PNNL) operated by Battelle for the U.S. Department of Energy under Contract No. DE-AC05–76RL01830. A portion of the microscopy was performed in the Radiological Microscopy Suite, located in the Radiochemical Processing Laboratory at PNNL. This work was in part supported by the Department of Energy Minority Serving Institution Partnership Program (MSIPP) managed by the Savannah River National Laboratory under SRNS contract DE-AC09-08SR22470. This research used resources of the Advanced Photon Source, a U.S. Department of Energy (DOE) Office of Science User Facility operated for the DOE Office of Science by Argonne National Laboratory under Contract No. DE-AC02-06CH11357. We also acknowledge ‘2019 APS/IIT XAFS Summer School’ in Chicago, IL.
The authors declare no competing interests.
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Boglaienko, D., Soltis, J.A., Kukkadapu, R.K. et al. Spontaneous redox continuum reveals sequestered technetium clusters and retarded mineral transformation of iron. Commun Chem 3, 87 (2020). https://doi.org/10.1038/s42004-020-0334-x