Abstract
Bastnäsite ((Ce,La)FCO3) is the primary mineral source of light rare earth elements, but its surface structure is not well understood. This presents a major challenge in improving beneficiation strategies. In this work, a synergistic combination of X-ray scattering and ab initio molecular dynamics (AIMD) was used to gain atomistic insight into the interfacial structure of bastnäsite. Surface X-ray scattering was used to measure crystal truncation rods (CTRs) of the bastnäsite (001) surface, a significant crystal face with a previously unknown termination. The best-fit atomic-scale model of the CTR data features a carbonate layer at the surface, which is stabilized by the relaxation of carbonate groups from their bulk structural positions. AIMD simulations predict similar surface relaxations, which are shown to be influenced by the protonation of oxygen atoms at the surface. Evidence of ordered water at the interface is also observed in the best-fit model and AIMD simulations. The presence of a carbonate layer at this dominant crystal surface is significant for improving separation technologies because most commonly used ligands utilize anionic functional groups to chelate metal cations at particle surfaces. Without modification, anionic ligands are expected to have poor affinity for the carbonate-terminated (001) surface.
Original language | English |
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Pages (from-to) | 21150-21160 |
Number of pages | 11 |
Journal | Journal of Physical Chemistry C |
Volume | 127 |
Issue number | 43 |
DOIs | |
State | Published - Nov 2 2023 |
Funding
AIMD and preliminary CTR data collection was supported by the Critical Materials Institute, an Energy Innovation Hub funded by the U.Ss Department of Energy (Subaward No. DE-AC02-07CH11358), Office of Energy Efficiency and Renewable Energy, Advanced Manufacturing Office. Analysis, final CTR data collection, and paper writing was supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, Chemical Sciences, Geosciences, and Biosciences Division. This research used resources of the Oak Ridge Leadership Computing Facility at the Oak Ridge National Laboratory, which is supported by the Office of Science of the U.S. Department of Energy under Contract No. DE-AC05-00OR22725, as well as resources of the National Energy Research Scientific Computing Center (NERSC), a U.S. Department of Energy Office of Science User Facility located at Lawrence Berkeley National Laboratory, operated under Contract No. DE-AC02-05CH11231 using NERSC award NP-ERCAP0020535. This manuscript has been authored by UT-Battelle, LLC, under Contract No. DE-AC05-00OR22725 with the U.S. Department of Energy. CTR measurements were conducted at GeoSoilEnviroCARS (The University of Chicago, Beamline 13-BM-C), Advanced Photon Source (APS), Argonne National Laboratory. GeoSoilEnviroCARS is supported by the National Science Foundation-Earth Sciences (EAR-1634415). A.K.W, J.E.S., and P.J.E. received further support for this work from the Department of Energy-GeoScience (DE-SC0019108). This research used resources of the Advanced Photon Source, a U.S. Department of Energy Office of Science User Facility operated for the DOE Office of Science by Argonne National Laboratory under Contract DE-AC02-06CH11357. Fitting of CTR data was completed using resources provided by the University of Chicago’s Research Computing Center.
Funders | Funder number |
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Critical Materials Institute | |
Department of Energy-GeoScience | DE-SC0019108 |
National Science Foundation-Earth Sciences | EAR-1634415 |
U.S. Department of Energy | DE-AC02-07CH11358 |
Advanced Manufacturing Office | |
Office of Science | |
Office of Energy Efficiency and Renewable Energy | |
Basic Energy Sciences | |
Argonne National Laboratory | DE-AC02-06CH11357 |
Lawrence Berkeley National Laboratory | DE-AC02-05CH11231, NP-ERCAP0020535 |
University of Chicago | |
Chemical Sciences, Geosciences, and Biosciences Division | DE-AC05-00OR22725 |