Magnetic anisotropy of dysprosium encapsulated metallofullerene molecules: a theoretical study

A series of metallofullerene single-ion magnets embedded with [DyO]<sup>+</sup> and [DyO<sub>2</sub>]<sup>-</sup> fragments were designed to probe the magnetic anisotropies and magnetic relaxation mechanisms using complete-active-space self-consistent field (CASSCF) calculations. CASSCF calculations showed that fullerenes with different diameters exert marginally varying influences on both the quantum tunneling of magnetization and energy level splitting, ultimately causing changes in energy barriers. Notably, [DyO]<sup>+</sup> encapsulated in the fullerenes of C<sub>80</sub> shows the best behavior. For [DyO<sub>2</sub>]<sup>-</sup>, however, the largest C<sub>100</sub> is preferable due to the presence of the largest O-Dy-O angle. If the O-Dy-O angle is increased to 180°, the energy barrier of [DyO<sub>2</sub>@C<sub>100</sub>]<sup>-</sup> would reach the highest value up to 4075.9 cm<sup>-1</sup>.

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Publication Details

Journal
Dalton Transactions
Published
2025-01-01
DOI
https://doi.org/10.1039/d5dt01279a
Primary Topic
Fullerene Chemistry and Applications
Type
article
Field-Weighted Citation Impact
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article

Magnetic anisotropy of dysprosium encapsulated metallofullerene molecules: a theoretical study

Yi‐Quan Zhang, Xiaole Zhang, Qi Ma, Dong-Mei Zhu et al.
3 links
Dalton Transactions
Fullerene Chemistry and Applications
article

Magnetic anisotropy of dysprosium encapsulated metallofullerene molecules: a theoretical study

Yi‐Quan Zhang, Xiaole Zhang, Qi Ma, Dong-Mei Zhu, Fang Lu
article en

Abstract

A series of metallofullerene single-ion magnets embedded with [DyO]<sup>+</sup> and [DyO<sub>2</sub>]<sup>-</sup> fragments were designed to probe the magnetic anisotropies and magnetic relaxation mechanisms using complete-active-space self-consistent field (CASSCF) calculations. CASSCF calculations showed that fullerenes with different diameters exert marginally varying influences on both the quantum tunneling of magnetization and energy level splitting, ultimately causing changes in energy barriers. Notably, [DyO]<sup>+</sup> encapsulated in the fullerenes of C<sub>80</sub> shows the best behavior. For [DyO<sub>2</sub>]<sup>-</sup>, however, the largest C<sub>100</sub> is preferable due to the presence of the largest O-Dy-O angle. If the O-Dy-O angle is increased to 180°, the energy barrier of [DyO<sub>2</sub>@C<sub>100</sub>]<sup>-</sup> would reach the highest value up to 4075.9 cm<sup>-1</sup>.

Dalton TransactionsVol. 54(34)
Nanjing Normal University (CN)
Openalex Percentile: Top 86%
Fullerene Chemistry and Applications
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