Ground and excited state charge transfer at aqueous nanodiamonds

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dc.identifier.uri http://dx.doi.org/10.15488/17129
dc.identifier.uri https://www.repo.uni-hannover.de/handle/123456789/17257
dc.contributor.author Kirschbaum, Thorren
dc.contributor.author Wang, Xiangfei
dc.contributor.author Bande, Annika
dc.date.accessioned 2024-04-18T06:09:21Z
dc.date.available 2024-04-18T06:09:21Z
dc.date.issued 2023
dc.identifier.citation Kirschbaum, T.; Wang, X.; Bande, A.: Ground and excited state charge transfer at aqueous nanodiamonds. In: Journal of Computational Chemistry 45 (2024), Nr. 11, S. 710-718. DOI: https://doi.org/10.1002/jcc.27279
dc.description.abstract Nanodiamonds (NDs) are unique carbonaceous materials with exceptionally high stability, hardness, and notable electronic properties. Their applications in photocatalysis, biomedicine, and energy materials are usually carried out in aqueous environments, where they interact with aqueous adsorbates. Especially, electron density may rearrange from the diamond material toward oxidative adsorbates such as oxygen, which is known as charge transfer doping. In this article, we quantify the charge transfer doping for NDs with inhomogeneous surface coverings (hydroxyl, fluorine, and amorphous carbon), as well as NDs doped with heteroatoms (B, Si, N) using hybrid density functional theory (DFT) calculations. The transfer doping magnitude is largely determined by the NDs' highest occupied molecular orbital energies, which can in turn be modified by the surface covering and doping. However, local modifications of the ND structures do not have any local effects on the magnitude of the charge transfer. We furthermore analyze the impact of aqueous adsorbates on the excited states of an aqueous ND in the context of photocatalysis via time-dependent DFT. Here, we find that the excited electrons are biased to move in the direction of the respective oxidative adsorbate. Surprisingly, we find that also unreactive species such as nitrous oxide may attract the excited electrons, which is probably due to the positive partial charge that is induced by the local N (Formula presented.) O solvation geometry. eng
dc.language.iso eng
dc.publisher New York, NY [u.a.] : Wiley
dc.relation.ispartofseries Journal of Computational Chemistry 45 (2024), Nr. 11
dc.rights CC BY 4.0 Unported
dc.rights.uri https://creativecommons.org/licenses/by/4.0
dc.subject DFT eng
dc.subject excited states eng
dc.subject molecular modeling eng
dc.subject nanodiamonds eng
dc.subject transfer doping eng
dc.subject.ddc 540 | Chemie
dc.title Ground and excited state charge transfer at aqueous nanodiamonds eng
dc.type Article
dc.type Text
dc.relation.essn 1096-987X
dc.relation.issn 0192-8651
dc.relation.doi https://doi.org/10.1002/jcc.27279
dc.bibliographicCitation.issue 11
dc.bibliographicCitation.volume 45
dc.bibliographicCitation.date 2024
dc.bibliographicCitation.firstPage 710
dc.bibliographicCitation.lastPage 718
dc.description.version publishedVersion eng
tib.accessRights frei zug�nglich


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