Thirty Years of Hide-and-Seek:\nCapturing Abundant\nbut Elusive M<sup>III</sup>@<i>C</i><sub>3<i>v</i></sub>(8)‑C<sub>82</sub> Isomer, and the Study of Magnetic\nAnisotropy Induced in Dy<

Our knowledge about endohedral metallofullerenes (EMFs)\nis restricted\nto the structures with sufficient kinetic stability to be extracted\nfrom the arc-discharge soot and processed by chromatographic and structural\ntechniques. For the most abundant rare-earth monometallofullerene\nM<sup>III</sup>@C<sub>82</sub>, experimental studies repeatedly demonstrated <i>C</i><sub>2<i>v</i></sub>(9) and <i>C</i><sub><i>s</i></sub>(6) carbon cage isomers, while computations\npredicted equal stability of the “missing” <i>C</i><sub>3<i>v</i></sub>(8) isomer. Here we report that this\nisomer is indeed formed but has not been recovered from soot using\nstandard protocols. Using a combination of redox extraction and subsequent\nbenzylation and trifluoromethylation with single-crystal XRD analysis\nof CF<sub>3</sub> adduct, we prove that Dy@<i>C</i><sub>3<i>v</i></sub>(8)-C<sub>82</sub> is one of the most abundantly\nproduced metallofullerenes, which was not identified in earlier studies\nbecause of the low kinetic stability. Further, using the Dy@<i>C</i><sub>3<i>v</i></sub>(8)-C<sub>82</sub>(CF<sub>3</sub>) and Dy@<i>C</i><sub>3<i>v</i></sub>(8)-C<sub>82</sub>(CH<sub>2</sub>Ph) monoadducts for the case study, we analyzed\nthe role of metal-fullerene bonding on the single-ion magnetic anisotropy\nof Dy in EMFs. The multitechnique approach, combining <i>ab initio</i> calculations, EPR spectroscopy, and SQUID magnetometry, demonstrated\nthat coordination of the Dy ion to the fullerene cage induces moderate,\nnonaxial, and very fluid magnetic anisotropy, which strongly varies\nwith small alterations in the Dy-fullerene coordination geometry.\nAs a result, Dy@<i>C</i><sub>3<i>v</i></sub>(8)-C<sub>82</sub>(CH<sub>2</sub>Ph) is a weak field-induced single-molecule\nmagnet (SMM), whose signatures of magnetic relaxation are detectable\nonly below 3 K. Our results demonstrate that metal-cage interactions\nshould have a detrimental effect on the SMM performance of EMFs. At\nthe same time, the strong variability of the magnetic anisotropy with\nmetal position suggests tunability and offers strategies for future\nprogress.

Publication Details

Journal
Figshare
Published
2024-09-02
DOI
https://doi.org/10.1021/jacs.4c10050.s001
Primary Topic
Fullerene Chemistry and Applications
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article
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article

Thirty Years of Hide-and-Seek:\nCapturing Abundant\nbut Elusive MIII@C3v(8)‑C82 Isomer, and the Study of Magnetic\nAnisotropy Induced in Dy<

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Fullerene Chemistry and Applications
article

Thirty Years of Hide-and-Seek:\nCapturing Abundant\nbut Elusive MIII@C3v(8)‑C82 Isomer, and the Study of Magnetic\nAnisotropy Induced in Dy<

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Abstract

Our knowledge about endohedral metallofullerenes (EMFs)\nis restricted\nto the structures with sufficient kinetic stability to be extracted\nfrom the arc-discharge soot and processed by chromatographic and structural\ntechniques. For the most abundant rare-earth monometallofullerene\nM&lt;sup&gt;III&lt;/sup&gt;@C&lt;sub&gt;82&lt;/sub&gt;, experimental studies repeatedly demonstrated &lt;i&gt;C&lt;/i&gt;&lt;sub&gt;2&lt;i&gt;v&lt;/i&gt;&lt;/sub&gt;(9) and &lt;i&gt;C&lt;/i&gt;&lt;sub&gt;&lt;i&gt;s&lt;/i&gt;&lt;/sub&gt;(6) carbon cage isomers, while computations\npredicted equal stability of the “missing” &lt;i&gt;C&lt;/i&gt;&lt;sub&gt;3&lt;i&gt;v&lt;/i&gt;&lt;/sub&gt;(8) isomer. Here we report that this\nisomer is indeed formed but has not been recovered from soot using\nstandard protocols. Using a combination of redox extraction and subsequent\nbenzylation and trifluoromethylation with single-crystal XRD analysis\nof CF&lt;sub&gt;3&lt;/sub&gt; adduct, we prove that Dy@&lt;i&gt;C&lt;/i&gt;&lt;sub&gt;3&lt;i&gt;v&lt;/i&gt;&lt;/sub&gt;(8)-C&lt;sub&gt;82&lt;/sub&gt; is one of the most abundantly\nproduced metallofullerenes, which was not identified in earlier studies\nbecause of the low kinetic stability. Further, using the Dy@&lt;i&gt;C&lt;/i&gt;&lt;sub&gt;3&lt;i&gt;v&lt;/i&gt;&lt;/sub&gt;(8)-C&lt;sub&gt;82&lt;/sub&gt;(CF&lt;sub&gt;3&lt;/sub&gt;) and Dy@&lt;i&gt;C&lt;/i&gt;&lt;sub&gt;3&lt;i&gt;v&lt;/i&gt;&lt;/sub&gt;(8)-C&lt;sub&gt;82&lt;/sub&gt;(CH&lt;sub&gt;2&lt;/sub&gt;Ph) monoadducts for the case study, we analyzed\nthe role of metal-fullerene bonding on the single-ion magnetic anisotropy\nof Dy in EMFs. The multitechnique approach, combining &lt;i&gt;ab initio&lt;/i&gt; calculations, EPR spectroscopy, and SQUID magnetometry, demonstrated\nthat coordination of the Dy ion to the fullerene cage induces moderate,\nnonaxial, and very fluid magnetic anisotropy, which strongly varies\nwith small alterations in the Dy-fullerene coordination geometry.\nAs a result, Dy@&lt;i&gt;C&lt;/i&gt;&lt;sub&gt;3&lt;i&gt;v&lt;/i&gt;&lt;/sub&gt;(8)-C&lt;sub&gt;82&lt;/sub&gt;(CH&lt;sub&gt;2&lt;/sub&gt;Ph) is a weak field-induced single-molecule\nmagnet (SMM), whose signatures of magnetic relaxation are detectable\nonly below 3 K. Our results demonstrate that metal-cage interactions\nshould have a detrimental effect on the SMM performance of EMFs. At\nthe same time, the strong variability of the magnetic anisotropy with\nmetal position suggests tunability and offers strategies for future\nprogress.

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