AVS 72 Session AC-FrM: Actinides and Rare Earths Science

Plutonium production for the U.S. weapons program at the Department of Energy’s Hanford Site created one of the world’s largest environmental remediation challenges. Cleanup of 200 million liters of radioactive and chemically complex waste stored in 177 underground tanks will take decades and cost billions of dollars. Addressing the sources and sinks of environmental radioactivity requires: (i) characterization of radioactive tank waste chemistry and (ii) understanding contaminant transport and reactivity in the subsurface. The Ion Dynamics in Radioactive Environments and Materials (IDREAM) Energy Frontier Research Center provides mechanistic insights into precipitation and dissolution processes central to Hanford tank waste treatment. Hanford sludge contains water-insoluble aluminum oxides/ hydroxides that influence waste processing. Atomic force microscopy (AFM) showed that gibbsite dissolution in alkaline solutions proceeds through release of aluminate dimers rather than classical monomer detachment mechanisms. Gibbsite can also selectively adsorb or incorporate rare earth elements in tank waste. IDREAM developed an AFM integrated with an X-ray source to directly observe radiolytically driven interfacial reactions with unprecedented spatial resolution. These studies revealed how ionizing radiation, adsorbed water, and surface impurities alter mineral reactivity under highly alkaline conditions. Adsorbed carboxylates or chromium on boehmite nanoplates significantly slowed dissolution despite incomplete surface coverage. In parallel with tank waste retrieval, legacy disposal to cribs and trenches during plutonium separations operations produced vadose zone contamination and groundwater plumes that continue to impact the environment. Key groundwater contaminants include technetium-99, present as highly mobile pertechnetate (TcO₄^-), and uranium. Current remediation strategies include treatment of perched water zones and permeable reactive barriers. Technologies under evaluation include tin apatite particles, sulfur-modified iron particles, bismuth subnitrate particles, calcium polysulfide, and polyphosphate amendments. Proposed immobilization mechanisms include reduction, adsorption, incorporation into mineral phases, and in situ precipitation/coating reactions. Their effectiveness for sequestration of Tc-99 and uranium was evaluated through batch and column studies using Hanford sediments. Advances in understanding radioactive waste chemistry, radiolytic interfacial processes, and contaminant immobilization mechanisms are critical for reducing environmental risks associated with Hanford waste retrieval, treatment, and disposal.

The discovery of local-moment magnetism in van der Waals (vdW) semiconductors down to the single-layer limit has led to a paradigm shift in the understanding of two-dimensional (2D) magnets and unleashed their potential for applications in microelectronic and optoelectronic devices. The incorporation of strong electronic and magnetic correlations in 2D vdW metals remains a sought-after platform not only to enable control of emergent quantum phases, such as superconductivity, but also to achieve more theoretically tractable microscopic models of complex materials. To date, however, there is limited success in the discovery of such metallic vdW platforms, and f-electron monolayers remain out of reach. In this talk, I will discuss experimental and theoretical studies of β-UTe₃, an actinide ferromagnet that can be exfoliated to the monolayer limit. A sizable electronic specific heat coefficient provides the hallmark of strong correlations. Remarkably, β-UTe₃ remains ferromagnetic in the half-unit-cell limit with an enhanced ordering temperature of 35 K, a factor of two larger than its bulk counterpart. Time permitting, I will also share recent spectroscopic insights into this system. Our work establishes β-UTe₃ as a novel materials platform for investigating and modeling correlated behavior in the monolayer limit and opens numerous avenues for quantum control with, e.g., strain engineering.

I will discuss modeling of the high-energy-resolution x-ray absorption and the resonant inelastic x-ray scattering in actinide compounds by means of the charge-transfer multiplet theory, that is, using the Anderson impurity model constructed on the basis of first-principles electronic-structure calculations. As one of the applications, I will analyze uranium L₃ and M₄ x-ray absorption spectra taken on UPd₂Cd₂₀. These spectra indicate that the uranium 5f shell undergoes valence fluctuations in this compound [1].

The regime of valence fluctuations, known from intermetallics based on the anomalous rare-earth elements (such as Ce, Yb, Sm, Eu), has not yet been identified by microscopic techniques in any uranium compound. It was only suggested in a few of them on the basis of thermodynamic properties (such as the magnetic susceptibility) and on their similarity to the properties of the rare-earth valence fluctuators [2]. Such arguments, however, are hardly unequivocal. The x-ray absorption spectroscopy certainly provides a more direct probe of the 5f-shell behavior. Although UPd₂Cd₂₀ has only one type of uranium site in its primitive cell, the absorption spectra obtained in the high-energy-resolution fluorescence-detection (HERFD) mode display two edges, each of which can be associated with a different valence state, 5f² and 5f³. The shape of the L₃ spectrum is well approximated by two shifted copies of the uranium 6d density of states obtained in density-functional calculations, the shape of the M₄ spectrum is well approximated by a combination of UCl₃ (5f³) and UCl₄ (5f²) spectra reported previously [3]. This points to the 5f² ↔ 5f³ fluctuations on a timescale longer than the characteristic time of the spectroscopy technique. Unlike 4f systems, in which such fluctuations typically lead to a destruction of magnetism due to one of the involved 4fⁿ configurations being non-magnetic [4], the 5f² and 5f³ states are both magnetic, allowing for a magnetic ordering in the fluctuating state—UPd₂Cd₂₀, in particular, is antiferromagnetic.

1. Y. Hirose et al., Experimental observation of valence fluctuations by high-resolution x-ray absorption spectroscopy in UPd₂Cd₂₀, Phys. Rev. B (2026), DOI: 10.1103/g9y8-7lq9
2. R. Troć, The possibility of the mixed valence state in the uranium intermetallic compounds: UCoGa₅, U₂Ru₂Sn and U₂RuGa₈. The scaling properties, J. Alloys Compd. 442, 34 (2007).
3. C. L. Silva at al., On the origin of low-valent uranium oxidation state, Nat. Commun. 15, 6861 (2024).
4. D. I. Khomskiĭ, The problem of intermediate valency, Sov. Phys. Usp. 22, 879 (1979).

The magnetic properties of tetravalent actinide centers differ markedly within the actinide row and with isoelectronic counterparts from the lanthanide row. Notable examples include the temperature independent paramagnetism of PuO₂,^1,2 exotic forms of multipolar order in UO₂ and NpO₂,^3,4 and the existence of multiple magnetic transitions in UF₄ and NpF₄.⁵ These studies have provided definitive evidence that the assignment of the valence electrons of actinides to 5f orbitals oversimplifies the underlying electronic structure. With magnetic resonance spectroscopic techniques we have shown that local magnetic and electric fields at ligand sites and the metal itself can be measured in the solid state with better than part per thousand resolution. We apply this approach in systematic studies of electronic structure in an isomorphous series of An(IV) compounds including the tetrafluorides (Fig. 1)^6,7 and the dioxides (Fig. 2).⁸ Plutonium, which is positioned in the 5f row between the light actinides -- characterized by itinerant valence electrons -- and higher Z elements that have valence electrons found to be in localized (atom-like) states, presents examples of both types of behavior.

REFERENCES

1. Raphael, G.; Lallement, R. Solid State Commun. 1968, 6, 383−385.
2. Gendron, F.; Autschbach, J. J. Phys. Chem. Lett. 2017, 8, 673−678.
3. Santini, P.; Carretta, S.; Amoretti, G.; Caciuffo, R.; Magnani, N.; Lander, G. H. Rev. Mod. Phys. 2009, 81, 807−863.
4. Rai, B. K.; Bretaña, A.; Morrison, G.; Greer, R.; Gofryk, K.; zur Loye, H.-C. Rep. Prog. Phys. 2024, 87, 066501.
5. Kern, S.; Hayward, J.; Roberts, S.; Richardson, J. W.; Rotella, F. J.; Soderholm, L.; Cort, B.; Tinkle, M.; West, M.; Hoisington, D.; Lander, G. H. J. Chem. Phys. 1994, 101, 9333–9337.
6. Capan, C.; Dempsey, R. J.; Sinkov, S.; McNamara, B.; Cho, H.; Phys. Rev. B 2016, 93, 224409.
7. Walter, E. D.; Capan, C.; Casella, A. J.; Carter, J. C.; McNamara, B. K.; Soderquist, C. Z.; Sinkov, S. I.; Clark, R. A.; Heller, F. D.; Sweet, L. E.; Corbey, J. F.; Cho, H. J. Chem. Phys. 2021, 154, 211101.
8. Rana, K.; Anand, K.; Park, S.; Sinkov, S. I.; Sweet, L. E; Cho, H. Inorg. Chem. 2025, 64, 21791-21795.

Despite occurring in nature, the chemistry of protactinium remains relatively unstudied due to its low abundance, radioactivity, and difficulty of isolation. However, existing studies on protactinium reveal chemical behavior and electronic structure that is unique even amongst the actinides, and this behavior has been attributed to the relatively large radial extent of the Pa 5f orbitals in tandem with their similar energy to the Pa 6d orbitals. In this work, the nature of the involvement of the Pa 5f and 6d orbitals is probed using high-resolution X-ray spectroscopy (HR-XANES) and resonant inelastic X-ray scattering (RIXS) experiments at the Pa M_3,4-edges, which have been demonstrated to be valuable probes of actinide electronic structure. For these studies, K₂PaF₇ and Pa₂O₅·xH₂O were synthesized in the solid state and characterized using Pa L₃-edge EXAFS. The Pa M_3,4-edge HR-XANES and RIXS experiments on these samples were conducted using two different scattering geometries and reveal dramatic differences in Pa 5f and 6d molecular orbital energetics and bond covalency between these coordination environments. We relate these differences to the competing influences of orbital energy and orbital overlap. These results form a basis of understanding for the electronic structure and chemistry of more complex Pa systems and demonstrate the high potential of the Pa 5f and 6d orbitals to participate in bonding interactions. The first experimental results on Ac M₃-edge HR-XANES of Ac-DOTA, relevant for understanding the bonding properties of Ac in radiopharmaceuticals, will also be presented and discussed. All experiments were conducted at the ACT end station of the CAT-ACT beamline at the KIT Light Source in Karlsruhe, Germany.

The capability to conduct x-ray synchrotron radiation spectroscopy on actinide materials has led to marked improvement in the fundamental understanding of f-electron behavior and chemistry of f-electron materials. Specialized beamlines and endstations capable of utilizing the unique spatial resolution, energy resolution, and intensity provided by the advent of near and third generation synchrotron radiation x-ray beams from storage ring user facilities, coupled to new sample holding techniques, has provided unmatched opportunities to characterize the chemical and physical properties for a range of actinide materials. This has been particularly evident in the soft x-ray region of synchrotron radiation where the scanning transmission x-ray microscope (STXM) has been used to determine electronic structure from the ligand perspective via ligand K-edge spectroscopy and resonant inelastic x-ray scattering (RIXS) has been employed to garner information about actinide metal centers Both have emerged as uniquely powerful tools to elucidate the electronic structure of actinide materials.

The results of recent actinide soft x-ray STXM and RIXS studies will be presented. These will include recent studies of the actinyl tris(benzoate) complexes with a range of donating/withdrawing substituents studied using scanning transmission x-ray microscopy (STXM) and time dependent density functional theory (TDDFT). The results from RIXS studies of the Am oxides will be recapped and prospects for future studies highlighted. Lastly, an update on the status of the laboratory-based x-ray absorption system used for f-element studies at LBNL will be presented.

Light-actinide magnetism is based on 5f electronic states, which are typically involved in metallic bonding, in contrast with the localized 4f states in lanthanides. Hence they are rather an analogy to transition-metal 3d materials, characterized by itinerant character. There is, however, a special ingredient in actinides, the strong spin-orbit interaction. It gives rise to orbital magnetic moments, yielding the strong anchor to the crystal lattice, providing thus new functionalities, as enormous magnetocrystalline anisotropy or giant magnetoresistance effects.

However, weaker Coulomb U restricts the 5f magnetism to the low temperature range. Combining with 3d metals, efficiently enhancing ordering temperatures in compounds with rare earths, does not work with actinides, as the 3d and 5f band states coexist at similar energies and hybridize between each other, suppressing typically both 3d and 5f magnetism.

There exists an alternative route of further reducing the 5f delocalization in compounds with large U-U spacings and weak 5f-ligand hybridization. The trick is to use polar bonding to reduce also the 5f-6d hybridization by withdrawing the U-6d states from the energy range of 5f’s by the bonding to an anion in Zintl phases. The most successful case is UCu₂P₂, a layered compounds with trigonal crystal structure, formed by alternating slabs of U (cation) and Cu-P (polyanion). The interactions can be further tuned by hydrostatic pressure, increasing the Curie temperature from 216 K to 296 K at pressures reaching 15 GPa. To describe variations of Curie temperature and spin and orbital moments, we applied X-ray magnetic circular dichroism at U-M_4,5 edges (ID 12 at ESRF) using perforated diamond anvil cells, minimizing the absorption in diamond. The results are in a good agreement with ab-initio calculations by means of the GGA+U method, which reveal other surprising features of the compound.

This work was supported by the Czech Science foundation under grant No. 25-16339S.

Heavy-fermion systems with magnetic ions in non-centrosymmetric sites have gained high attention during the past years. A prominent example is CeRh2As2 which exhibits a complex phase diagram with many unusual phases [1,2]. Theoretical discussions mainly focused on the role of the Rashba effect, i. e., on the consequences of local inversion symmetry breaking on the spins of the heavy quasiparticles [3].

In the present contribution, I will discuss consequences of local inversion symmetry breaking on the orbital degrees of freedom, i. e., the possible hybridization of orbitals with different parities. The inter-site interaction resulting from local Ce 4f-Ce 5d hybridization and d-d- hopping can lead to new cooperative phenomena like the lattice instability in CeCoSi [4].

I will discuss the consequences of these cooperative phenomena for the Raman spectra of CeCoSi [5].

[1] S. Khim et al, Science 373, 1012 (2021)

[2] D. Hafner et al, Phys. Rev. X 12, 011023 (2022)

[3] see e. g. B. K. Nally and P. M. R. Brydon, New J. Phys. 26, 093015 (2024) and references therein

[4] Takeshi Matsumura et al., Phys. Rev. B 113, 014415 (2026)

[5] Owen Moulding et al., arXiv: 2505.03249

Accurate fissile isotope identification using Fission Track Analysis (FTA) is fundamentally limited by stochastic variations in individual fission-fragment trajectories and by the finite statistics obtainable from single-cluster measurements. While recent advances in automated image processing and synthetic-data-driven reconstruction have improved the robustness of FTA, isotopic discrimination between fissile materials with similar fission-fragment distributions remains challenging.

In this work, we propose a novel statistical enhancement framework based on superposition of reconstructed fission-track clusters originating from the same fissile grain. The method combines multiple realizations of track topologies into a unified statistical representation, effectively increasing counting statistics without increasing detector area or irradiation complexity.

Monte Carlo simulations using Geant4 were performed for ²³⁵U, ²³³U, and ²²⁹Th embedded in aerogel-assisted LEXAN® solid-state nuclear track detectors (SSNTDs). Synthetic microscope images were generated and processed using an automated reconstruction pipeline to extract track morphology, cluster centroids, and Real Flight Path (RFP) distributions.

Statistical analysis demonstrated that the proposed superposition framework reduces stochastic uncertainty approximately according to: σ_eff = 1/√N

where N is the number of superposed cluster realizations. For example, superposition of N = 9 realizations improves discrimination between ²³⁵U and ²²⁹Th from ~3σ to ~9σ, and between ²³⁵U and ²³³U from ~1σ to ~3σ, consistent with the expected √N scaling. More distinct isotope pairs exhibited even stronger enhancement, exceeding 5σ significance for modest superposition levels.

The proposed methodology transforms FTA from a primarily single-event morphological analysis into an ensemble-based statistical fingerprinting technique. This approach provides a scalable pathway toward improved isotopic sensitivity, automated nuclear forensic analysis, and enhanced safeguards verification, particularly for isotopes with partially overlapping fission-fragment signatures.

Future work will focus on experimental validation under neutron irradiation conditions and implementation of physics-informed alignment algorithms for real detector datasets.