Exploring Anomalous Photoelectron Angular Distributions in the Photoelectron Spectra of Gd <sub>3</sub> O <sub>3</sub> <sup>–</sup> : Study of Gd <sub>3</sub> O <sub>2</sub> <sup>–</sup> and Gd <sub>3</sub> O <sub>3</sub> <sup>–</sup> Using Photoelec

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 Gd<sub>3</sub>O<sub>2</sub><sup>-</sup> and Gd<sub>3</sub>O<sub>3</sub><sup>-</sup>, 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 Gd<sub>3</sub>O<sub>2</sub> is measured to be 1.29 ± 0.05 eV, and that of Gd<sub>3</sub>O<sub>3</sub> 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 Gd<sub>3</sub>O<sub>3</sub><sup>-</sup> in a way that suggests four different subgroups of transitions. Results of calculations on Gd<sub>3</sub>O<sub>2</sub><sup>-</sup> suggest kite or V-shape structures with antiferromagnetic coupling between one of the 4f<sup>7</sup> subshells with the two others. Calculations on Gd<sub>3</sub>O<sub>3</sub><sup>-</sup> 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 4f<sup>7</sup> 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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Journal
The Journal of Physical Chemistry A
Published
2025-12-03
DOI
https://doi.org/10.1021/acs.jpca.5c06858
Primary Topic
Luminescence Properties of Advanced Materials
Type
article
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Exploring Anomalous Photoelectron Angular Distributions in the Photoelectron Spectra of Gd 3 O 3 – : Study of Gd 3 O 2 – and Gd 3 O 3 – Using Photoelec

Lee M. Thompson, Ali Abou Taka, Caroline Chick Jarrold, Shivangi Vaish et al.
The Journal of Physical Chemistry A
Luminescence Properties of Advanced Materials
article

Exploring Anomalous Photoelectron Angular Distributions in the Photoelectron Spectra of Gd 3 O 3 – : Study of Gd 3 O 2 – and Gd 3 O 3 – Using Photoelec

Lee M. Thompson, Ali Abou Taka, Caroline Chick Jarrold, Shivangi Vaish, Catherine Dwyer, Caleb D. Huizenga, Hrant P. Hratchian, Andrew Bovill
article en

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 Gd<sub>3</sub>O<sub>2</sub><sup>-</sup> and Gd<sub>3</sub>O<sub>3</sub><sup>-</sup>, 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 Gd<sub>3</sub>O<sub>2</sub> is measured to be 1.29 ± 0.05 eV, and that of Gd<sub>3</sub>O<sub>3</sub> 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 Gd<sub>3</sub>O<sub>3</sub><sup>-</sup> in a way that suggests four different subgroups of transitions. Results of calculations on Gd<sub>3</sub>O<sub>2</sub><sup>-</sup> suggest kite or V-shape structures with antiferromagnetic coupling between one of the 4f<sup>7</sup> subshells with the two others. Calculations on Gd<sub>3</sub>O<sub>3</sub><sup>-</sup> 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 4f<sup>7</sup> 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.

The Journal of Physical Chemistry AVol. 129(50)
University of Louisville (US), University of California, Merced (US), Indiana University Bloomington (US), University of Louisville Hospital (US)
Openalex Percentile: Top 69%
Luminescence Properties of Advanced Materials
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