Ground and excited state charge transfer at aqueous nanodiamonds

Publikation: Beitrag in FachzeitschriftArtikelForschungPeer-Review

Autoren

  • Thorren Kirschbaum
  • Xiangfei Wang
  • Annika Bande

Organisationseinheiten

Externe Organisationen

  • Freie Universität Berlin (FU Berlin)
  • Helmholtz-Zentrum Berlin für Materialien und Energie GmbH
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Details

OriginalspracheEnglisch
Seiten (von - bis)710-718
Seitenumfang9
FachzeitschriftJournal of computational chemistry
Jahrgang45
Ausgabenummer11
PublikationsstatusVeröffentlicht - 15 März 2024

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.

Zitieren

Ground and excited state charge transfer at aqueous nanodiamonds. / Kirschbaum, Thorren; Wang, Xiangfei; Bande, Annika.
in: Journal of computational chemistry, Jahrgang 45, Nr. 11, 15.03.2024, S. 710-718.

Publikation: Beitrag in FachzeitschriftArtikelForschungPeer-Review

Kirschbaum T, Wang X, Bande A. Ground and excited state charge transfer at aqueous nanodiamonds. Journal of computational chemistry. 2024 Mär 15;45(11):710-718. doi: 10.1002/jcc.27279
Kirschbaum, Thorren ; Wang, Xiangfei ; Bande, Annika. / Ground and excited state charge transfer at aqueous nanodiamonds. in: Journal of computational chemistry. 2024 ; Jahrgang 45, Nr. 11. S. 710-718.
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AU - Wang, Xiangfei

AU - Bande, Annika

N1 - Funding Information: Thorren Kirschbaum acknowledges support from the HelmholtzEinstein International Berlin Research School in Data Science (HEI-BRiDS). Xiangfei Wang acknowledges funding from the China Scholar-ship Council. Computing resources were kindly provided by the FreieUniversität Berlin hpc cluster Curta.74Open Access funding enabledand organized by Projekt DEAL

PY - 2024/3/15

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N2 - 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.

AB - 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.

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