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Origin of the Unusual Ground-State Spin S = 9 in a Cr(10) Single-Molecule Magnet

[Image: see text] The molecular wheel [Cr(10)(OMe)(20)(O(2)CCMe(3))(10)], abbreviated {Cr(10)}, with an unusual intermediate total spin S = 9 and non-negligible cluster anisotropy, D/k(B) = −0.045(2) K, is a rare case among wheels based on an even number of 3d-metals, which usually present an antife...

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Autores principales: Rubín, Javier, Arauzo, Ana, Bartolomé, Elena, Sedona, Francesco, Rancan, Marzio, Armelao, Lidia, Luzón, Javier, Guidi, Tatiana, Garlatti, Elena, Wilhelm, Fabrice, Rogalev, Andrei, Amann, Andreas, Spagna, Stefano, Bartolomé, Juan, Bartolomé, Fernando
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2022
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9979690/
https://www.ncbi.nlm.nih.gov/pubmed/35759747
http://dx.doi.org/10.1021/jacs.2c05453
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author Rubín, Javier
Arauzo, Ana
Bartolomé, Elena
Sedona, Francesco
Rancan, Marzio
Armelao, Lidia
Luzón, Javier
Guidi, Tatiana
Garlatti, Elena
Wilhelm, Fabrice
Rogalev, Andrei
Amann, Andreas
Spagna, Stefano
Bartolomé, Juan
Bartolomé, Fernando
author_facet Rubín, Javier
Arauzo, Ana
Bartolomé, Elena
Sedona, Francesco
Rancan, Marzio
Armelao, Lidia
Luzón, Javier
Guidi, Tatiana
Garlatti, Elena
Wilhelm, Fabrice
Rogalev, Andrei
Amann, Andreas
Spagna, Stefano
Bartolomé, Juan
Bartolomé, Fernando
author_sort Rubín, Javier
collection PubMed
description [Image: see text] The molecular wheel [Cr(10)(OMe)(20)(O(2)CCMe(3))(10)], abbreviated {Cr(10)}, with an unusual intermediate total spin S = 9 and non-negligible cluster anisotropy, D/k(B) = −0.045(2) K, is a rare case among wheels based on an even number of 3d-metals, which usually present an antiferromagnetic (AF) ground state (S = 0). Herein, we unveil the origin of such a behavior. Angular magnetometry measurements performed on a single crystal confirmed the axial anisotropic behavior of {Cr(10)}. For powder samples, the temperature dependence of the susceptibility plotted as χT(T) showed an overall ferromagnetic (FM) behavior down to 1.8 K, whereas the magnetization curve M(H) did not saturate at the expected 30 μ(B)/fu for 10 FM coupled 3/2 spin Cr(3+) ions, but to a much lower value, corresponding to S = 9. In addition, the X-ray magnetic circular dichroism (XMCD) measured at high magnetic field (170 kOe) and 7.5 K showed the polarization of the cluster moment up to 23 μ(B)/fu. The magnetic results can be rationalized within a model, including the cluster anisotropy, in which the {Cr(10)} wheel is formed by two semiwheels, each with four Cr(3+) spins FM coupled (J(FM)/k(B) = 2.0 K), separated by two Cr(3+) ions AF coupled asymmetrically (J(23)/k(B) = J(78)/k(B) = −2.0 K; J(34)/k(B) = J(89)/k(B) = −0.25 K). Inelastic neutron scattering and heat capacity allowed us to confirm this model leading to the S = 9 ground state and first excited S = 8. Single-molecule magnet behavior with an activation energy of U/k(B) = 4.0(5) K in the absence of applied field was observed through ac susceptibility measurements down to 0.1 K. The intriguing magnetic behavior of {Cr(10)} arises from the detailed asymmetry in the molecule interactions produced by small-angle distortions in the angles of the Cr–O–Cr alkoxy bridges coupling the Cr(3+) ions, as demonstrated by ab initio and density functional theory calculations, while the cluster anisotropy can be correlated to the single-ion anisotropies calculated for each Cr(3+) ion in the wheel.
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spelling pubmed-99796902023-03-03 Origin of the Unusual Ground-State Spin S = 9 in a Cr(10) Single-Molecule Magnet Rubín, Javier Arauzo, Ana Bartolomé, Elena Sedona, Francesco Rancan, Marzio Armelao, Lidia Luzón, Javier Guidi, Tatiana Garlatti, Elena Wilhelm, Fabrice Rogalev, Andrei Amann, Andreas Spagna, Stefano Bartolomé, Juan Bartolomé, Fernando J Am Chem Soc [Image: see text] The molecular wheel [Cr(10)(OMe)(20)(O(2)CCMe(3))(10)], abbreviated {Cr(10)}, with an unusual intermediate total spin S = 9 and non-negligible cluster anisotropy, D/k(B) = −0.045(2) K, is a rare case among wheels based on an even number of 3d-metals, which usually present an antiferromagnetic (AF) ground state (S = 0). Herein, we unveil the origin of such a behavior. Angular magnetometry measurements performed on a single crystal confirmed the axial anisotropic behavior of {Cr(10)}. For powder samples, the temperature dependence of the susceptibility plotted as χT(T) showed an overall ferromagnetic (FM) behavior down to 1.8 K, whereas the magnetization curve M(H) did not saturate at the expected 30 μ(B)/fu for 10 FM coupled 3/2 spin Cr(3+) ions, but to a much lower value, corresponding to S = 9. In addition, the X-ray magnetic circular dichroism (XMCD) measured at high magnetic field (170 kOe) and 7.5 K showed the polarization of the cluster moment up to 23 μ(B)/fu. The magnetic results can be rationalized within a model, including the cluster anisotropy, in which the {Cr(10)} wheel is formed by two semiwheels, each with four Cr(3+) spins FM coupled (J(FM)/k(B) = 2.0 K), separated by two Cr(3+) ions AF coupled asymmetrically (J(23)/k(B) = J(78)/k(B) = −2.0 K; J(34)/k(B) = J(89)/k(B) = −0.25 K). Inelastic neutron scattering and heat capacity allowed us to confirm this model leading to the S = 9 ground state and first excited S = 8. Single-molecule magnet behavior with an activation energy of U/k(B) = 4.0(5) K in the absence of applied field was observed through ac susceptibility measurements down to 0.1 K. The intriguing magnetic behavior of {Cr(10)} arises from the detailed asymmetry in the molecule interactions produced by small-angle distortions in the angles of the Cr–O–Cr alkoxy bridges coupling the Cr(3+) ions, as demonstrated by ab initio and density functional theory calculations, while the cluster anisotropy can be correlated to the single-ion anisotropies calculated for each Cr(3+) ion in the wheel. American Chemical Society 2022-06-27 /pmc/articles/PMC9979690/ /pubmed/35759747 http://dx.doi.org/10.1021/jacs.2c05453 Text en © 2022 American Chemical Society https://creativecommons.org/licenses/by/4.0/Permits the broadest form of re-use including for commercial purposes, provided that author attribution and integrity are maintained (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Rubín, Javier
Arauzo, Ana
Bartolomé, Elena
Sedona, Francesco
Rancan, Marzio
Armelao, Lidia
Luzón, Javier
Guidi, Tatiana
Garlatti, Elena
Wilhelm, Fabrice
Rogalev, Andrei
Amann, Andreas
Spagna, Stefano
Bartolomé, Juan
Bartolomé, Fernando
Origin of the Unusual Ground-State Spin S = 9 in a Cr(10) Single-Molecule Magnet
title Origin of the Unusual Ground-State Spin S = 9 in a Cr(10) Single-Molecule Magnet
title_full Origin of the Unusual Ground-State Spin S = 9 in a Cr(10) Single-Molecule Magnet
title_fullStr Origin of the Unusual Ground-State Spin S = 9 in a Cr(10) Single-Molecule Magnet
title_full_unstemmed Origin of the Unusual Ground-State Spin S = 9 in a Cr(10) Single-Molecule Magnet
title_short Origin of the Unusual Ground-State Spin S = 9 in a Cr(10) Single-Molecule Magnet
title_sort origin of the unusual ground-state spin s = 9 in a cr(10) single-molecule magnet
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9979690/
https://www.ncbi.nlm.nih.gov/pubmed/35759747
http://dx.doi.org/10.1021/jacs.2c05453
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