Coordination Sphere of Lanthanide Aqua Ions Resolved with Ab Initio Molecular Dynamics and X-ray Absorption Spectroscopy

Richard C. Shiery, John L. Fulton, Mahalingam Balasubramanian, Manh Thuong Nguyen, Jun Bo Lu, Jun Li, Roger Rousseau, Vassiliki Alexandra Glezakou, David C. Cantu

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52 Scopus citations

Abstract

To resolve the fleeting structures of lanthanide Ln3+ aqua ions in solution, we (i) performed the first ab initio molecular dynamics (AIMD) simulations of the entire series of Ln3+ aqua ions in explicit water solvent using pseudopotentials and basis sets recently optimized for lanthanides and (ii) measured the symmetry of the hydrating waters about Ln3+ ions (Nd3+, Dy3+, Er3+, Lu3+) for the first time with extended X-ray absorption fine structure (EXAFS). EXAFS spectra were measured experimentally and generated from AIMD trajectories to directly compare simulation, which concurrently considers the electronic structure and the atomic dynamics in solution, with experiment. We performed a comprehensive evaluation of EXAFS multiple-scattering analysis (up to 6.5 Å) to measure Ln-O distances and angular correlations (i.e., symmetry) and elucidate the molecular geometry of the first hydration shell. This evaluation, in combination with symmetry-dependent L3- and L1-edge spectral analysis, shows that the AIMD simulations remarkably reproduces the experimental EXAFS data. The error in the predicted Ln-O distances is less than 0.07 Å for the later lanthanides, while we observed excellent agreement with predicted distances within experimental uncertainty for the early lanthanides. Our analysis revealed a dynamic, symmetrically disordered first coordination shell, which does not conform to a single molecular geometry for most lanthanides. This work sheds critical light on the highly elusive coordination geometry of the Ln3+ aqua ions.

Original languageEnglish
Pages (from-to)3117-3130
Number of pages14
JournalInorganic Chemistry
Volume60
Issue number5
DOIs
StatePublished - Mar 1 2021
Externally publishedYes

Funding

R.C.S. and D.C.C. acknowledge the donors of the American Chemical Society Petroleum Research Fund for partial support of this research, as well as the Vice President for Research and Innovation, and the College of Engineering, of the University of Nevada, Reno. Work by V.-A.G., M.-T.N., and R.R. was supported under project 72353, and J.L.F. under project 16248, funded by the U.S. Department of Energy (DOE), Office of Science, Office of Basic Energy Sciences, Division of Chemical Sciences, Geosciences, and Biosciences. Pacific Northwest National Laboratory (PNNL) is operated by Battelle for the U.S. DOE under Contract No. DE-AC05-76RL01830. This research used resources of the Advanced Photon Source, the 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. J.L. and J.B.L. are supported by the National Natural Science Foundation of China (grant no. 22033005) and Guangdong Provincial Key Laboratory of Catalysis (No. 2020B121201002). Calculations were performed in Pronghorn, the High-Performance Computing cluster of the University of Nevada, Reno, as well as in PNNL Research Computing clusters.

FundersFunder number
Basic Energy Sciences
American Chemical Society Petroleum Research Fund
U.S. Department of Energy
Office of Science
Guangdong Provincial Key Laboratory of Catalysis2020B121201002
Guangdong Provincial Key Laboratory of Catalysis
Argonne National LaboratoryDE-AC02-06CH11357
Argonne National Laboratory
Chemical Sciences, Geosciences, and Biosciences DivisionDE-AC05-76RL01830
Chemical Sciences, Geosciences, and Biosciences Division
National Natural Science Foundation of China22033005
National Natural Science Foundation of China
University of Nevada, Reno72353, 16248
University of Nevada, Reno

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