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Bounding [AnO 2 ] 2+ (An = U, Np) covalency by simulated O K-edge and An M-edge X-ray absorption near-edge spectroscopy †

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Bounding [AnO 2 ] 2+ (An = U, Np) covalency by simulated O K-edge and An M-edge X-ray absorption near-edge spectroscopy †. / Stanistreet-Welsh, Kurtis; Kerridge, Andrew.
In: Physical Chemistry Chemical Physics, Vol. 2023, No. 25, 21.09.2023, p. 3753-23760.

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Stanistreet-Welsh K, Kerridge A. Bounding [AnO 2 ] 2+ (An = U, Np) covalency by simulated O K-edge and An M-edge X-ray absorption near-edge spectroscopy †. Physical Chemistry Chemical Physics. 2023 Sept 21;2023(25):3753-23760. Epub 2023 Aug 24. doi: 10.1039/d3cp03149g

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Stanistreet-Welsh, Kurtis ; Kerridge, Andrew. / Bounding [AnO 2 ] 2+ (An = U, Np) covalency by simulated O K-edge and An M-edge X-ray absorption near-edge spectroscopy †. In: Physical Chemistry Chemical Physics. 2023 ; Vol. 2023, No. 25. pp. 3753-23760.

Bibtex

@article{719e91acf8594d068a80149cc7ca67b7,
title = "Bounding [AnO 2 ] 2+ (An = U, Np) covalency by simulated O K-edge and An M-edge X-ray absorption near-edge spectroscopy †",
abstract = "Restricted active space simulations are shown to accurately reproduce and characterise both O K-edge and U M -edge spectra of uranyl in excellent agreement with experimental peak positions and are extended to the Np analogue. Analysis of bonding orbital composition in the ground and O K-edge core-excited states demonstrates that metal contribution is underestimated in the latter. In contrast, An M -edge core-excited states produce bonding orbital compositions significantly more representative of those in the ground state. Quantum Theory of Atoms in Molecules analysis is employed to explain the discrepancy between K- and M-edge data and demonstrates that the location of the core-hole impacts the pattern of electron localisation in core-excited states. An apparent contradiction to this behaviour in neptunyl is rationalised in terms interelectronic repulsion between the unpaired 5f electron and the excited core-electron.",
author = "Kurtis Stanistreet-Welsh and Andrew Kerridge",
year = "2023",
month = sep,
day = "21",
doi = "10.1039/d3cp03149g",
language = "English",
volume = "2023",
pages = "3753--23760",
journal = "Physical Chemistry Chemical Physics",
issn = "1463-9076",
publisher = "Royal Society of Chemistry",
number = "25",

}

RIS

TY - JOUR

T1 - Bounding [AnO 2 ] 2+ (An = U, Np) covalency by simulated O K-edge and An M-edge X-ray absorption near-edge spectroscopy †

AU - Stanistreet-Welsh, Kurtis

AU - Kerridge, Andrew

PY - 2023/9/21

Y1 - 2023/9/21

N2 - Restricted active space simulations are shown to accurately reproduce and characterise both O K-edge and U M -edge spectra of uranyl in excellent agreement with experimental peak positions and are extended to the Np analogue. Analysis of bonding orbital composition in the ground and O K-edge core-excited states demonstrates that metal contribution is underestimated in the latter. In contrast, An M -edge core-excited states produce bonding orbital compositions significantly more representative of those in the ground state. Quantum Theory of Atoms in Molecules analysis is employed to explain the discrepancy between K- and M-edge data and demonstrates that the location of the core-hole impacts the pattern of electron localisation in core-excited states. An apparent contradiction to this behaviour in neptunyl is rationalised in terms interelectronic repulsion between the unpaired 5f electron and the excited core-electron.

AB - Restricted active space simulations are shown to accurately reproduce and characterise both O K-edge and U M -edge spectra of uranyl in excellent agreement with experimental peak positions and are extended to the Np analogue. Analysis of bonding orbital composition in the ground and O K-edge core-excited states demonstrates that metal contribution is underestimated in the latter. In contrast, An M -edge core-excited states produce bonding orbital compositions significantly more representative of those in the ground state. Quantum Theory of Atoms in Molecules analysis is employed to explain the discrepancy between K- and M-edge data and demonstrates that the location of the core-hole impacts the pattern of electron localisation in core-excited states. An apparent contradiction to this behaviour in neptunyl is rationalised in terms interelectronic repulsion between the unpaired 5f electron and the excited core-electron.

U2 - 10.1039/d3cp03149g

DO - 10.1039/d3cp03149g

M3 - Journal article

VL - 2023

SP - 3753

EP - 23760

JO - Physical Chemistry Chemical Physics

JF - Physical Chemistry Chemical Physics

SN - 1463-9076

IS - 25

ER -