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Updated: Jan 9, 2026

Photoelectron Imaging of Anions Illustrated by 310 Nm Detachment of F−
Published on: July 27, 2018
Exploring Anomalous Photoelectron Angular Distributions in the Photoelectron Spectra of Gd3O3-: Study of Gd3O2- and
Caleb D Huizenga1, Shivangi Vaish1, Christian Dwyer2
1Department of Chemistry, Indiana University, 800 East Kirkwood Avenue, Bloomington, Indiana 47405, United States.
Abstract:
Anion photoelectron (PE) spectra of lanthanide oxide clusters obtained previously have exhibited anomalous photoelectron angular distributions which were attributed to strong PE-valence electron (PEVE) interactions. To further explore this effect, we have obtained the PE spectra of Gd3O2- and Gd3O3-, two clusters that have similarly complex electronic structures but contrasting symmetries. The spectra exhibit manifolds of detachment transitions at similar binding energies in a 0.5 eV window of energy. The electron affinity of Gd3O2 is measured to be 1.29 ± 0.05 eV, and that of Gd3O3 is 1.31 ± 0.05 eV. As seen in previous studies on lanthanide oxide cluster anions in lower than conventional oxidation states, transitions in spectra obtained lower photon energies are more congested than those obtained with higher photon energy, a signature of strong PEVE interactions. While the detachment transitions have predominantly parallel photoelectron angular distributions (PAD), the PAD varies across the manifold of transitions in the PE spectrum of Gd3O3- in a way that suggests four different subgroups of transitions. Results of calculations on Gd3O2- suggest kite or V-shape structures with antiferromagnetic coupling between one of the 4f7 subshells with the two others. Calculations on Gd3O3- more definitively point to ring structures with a nearly isoenergetic ferromagnetically coupled high spin (24-tet) state and a dectet state in which one of the 4f7 subshells is antiferromagnetically coupled with the other two. Taking these results as qualitative, we propose that strong mixing between the unperturbed states predicted computationally leads to overlapping transitions with different PADs.
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