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Single‐Molecule Magnets DyM(2)N@C(80) and Dy(2)MN@C(80) (M=Sc, Lu): The Impact of Diamagnetic Metals on Dy(3+) Magnetic Anisotropy, Dy⋅⋅⋅Dy Coupling, and Mixing of Molecular and Lattice Vibrations

The substitution of scandium in fullerene single‐molecule magnets (SMMs) DySc(2)N@C(80) and Dy(2)ScN@C(80) by lutetium has been studied to explore the influence of the diamagnetic metal on the SMM performance of dysprosium nitride clusterfullerenes. The use of lutetium led to an improved SMM perform...

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Detalles Bibliográficos
Autores principales: Spree, Lukas, Schlesier, Christin, Kostanyan, Aram, Westerström, Rasmus, Greber, Thomas, Büchner, Bernd, Avdoshenko, Stanislav M., Popov, Alexey A.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: John Wiley and Sons Inc. 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7065109/
https://www.ncbi.nlm.nih.gov/pubmed/31774196
http://dx.doi.org/10.1002/chem.201904879
Descripción
Sumario:The substitution of scandium in fullerene single‐molecule magnets (SMMs) DySc(2)N@C(80) and Dy(2)ScN@C(80) by lutetium has been studied to explore the influence of the diamagnetic metal on the SMM performance of dysprosium nitride clusterfullerenes. The use of lutetium led to an improved SMM performance of DyLu(2)N@C(80), which shows a higher blocking temperature of magnetization (T (B)=9.5 K), longer relaxation times, and broader hysteresis than DySc(2)N@C(80) (T (B)=6.9 K). At the same time, Dy(2)LuN@C(80) was found to have a similar blocking temperature of magnetization to Dy(2)ScN@C(80) (T (B)=8 K), but substantially different interactions between the magnetic moments of the dysprosium ions in the Dy(2)MN clusters. Surprisingly, although the intramolecular dipolar interactions in Dy(2)LuN@C(80) and Dy(2)ScN@C(80) are of similar strength, the exchange interactions in Dy(2)LuN@C(80) are close to zero. Analysis of the low‐frequency molecular and lattice vibrations showed strong mixing of the lattice modes and endohedral cluster librations in k‐space. This mixing simplifies the spin–lattice relaxation by conserving the momentum during the spin flip and helping to distribute the moment and energy further into the lattice.