High-Coercivity Ferrimagnet Co₂FeO₂BO₃: XMCD Insights into Charge-Ordering and Cation Distribution

The multi-sublattice ferrimagnet Co<sub>2</sub>FeO<sub>2</sub>BO<sub>3</sub>, a prominent example of lanthanide-free magnets, was the subject of element-selective studies using X-ray magnetic circular dichroism (XMCD) observations at the <i>L</i>- and...

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Main Author: Mikhail S. Platunov
Format: Article
Language:English
Published: MDPI AG 2025-01-01
Series:Inorganics
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Online Access:https://www.mdpi.com/2304-6740/13/1/24
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author Mikhail S. Platunov
author_facet Mikhail S. Platunov
author_sort Mikhail S. Platunov
collection DOAJ
description The multi-sublattice ferrimagnet Co<sub>2</sub>FeO<sub>2</sub>BO<sub>3</sub>, a prominent example of lanthanide-free magnets, was the subject of element-selective studies using X-ray magnetic circular dichroism (XMCD) observations at the <i>L</i>- and <i>K</i>- X-ray absorption edges. Research findings indicate that the distinct magnetic characteristics of Co<sub>2</sub>FeO<sub>2</sub>BO<sub>3</sub>, namely its remarkable high coercivity (which surpasses 7 Tesla at low temperatures), originate from an atypical arrangement of magnetic ions in the crystal structure (sp.gr. <i>Pbam</i>). The antiferromagnetic nature of the Co<sup>2+</sup>-O-Fe<sup>3+</sup> exchange interaction was confirmed by identifying the spin and orbital contributions to the total magnetization from Co (m<sub>L</sub> = 0.27 ± 0.1 μ<sub>B</sub>/ion and m<sup>eff</sup><sub>S</sub> = 0.53 ± 0.1 μ<sub>B</sub>/ion) and Fe (m<sub>L</sub> = 0.05 ± 0.1 μ<sub>B</sub>/ion and m<sup>eff</sup><sub>S</sub> = 0.80 ± 0.1 μ<sub>B</sub>/ion) ions through element-selective XMCD analysis. Additionally, the research explicitly revealed that the strong magnetic anisotropy is a result of the significant unquenched orbital magnetic moment of Co, a feature that is also present in the related compound Co<sub>3</sub>O<sub>2</sub>BO<sub>3</sub>. A complex magnetic structure in Co<sub>2</sub>FeO<sub>2</sub>BO<sub>3</sub>, with infinite Co²⁺O<sub>6</sub> layers in the <b>bc</b>-plane and strong antiferromagnetic coupling through Fe<sup>3</sup>⁺ ions, is suggested by element-selective hysteresis data, which revealed that Co²⁺ ions contribute both antiferromagnetic and ferromagnetic components to the total magnetization. The findings underline the suitability of Co<sub>2</sub>FeO<sub>2</sub>BO<sub>3</sub> for applications in extreme environments, such as low temperatures and high magnetic fields, where its unique magnetic topology and anisotropy can be harnessed for advanced technologies, including materials for space exploration and quantum devices. This XMCD study opens the door to the production of novel high-coercivity, lanthanide-free magnetic materials by showing that targeted substitution at specific crystallographic sites can significantly enhance the magnetic properties of such materials.
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spelling doaj-art-8b62698d4edd4696af018174358a4e352025-01-24T13:35:31ZengMDPI AGInorganics2304-67402025-01-011312410.3390/inorganics13010024High-Coercivity Ferrimagnet Co₂FeO₂BO₃: XMCD Insights into Charge-Ordering and Cation DistributionMikhail S. Platunov0Synchrotron Radiation Facility SKIF, Kol’tsovo 630559, RussiaThe multi-sublattice ferrimagnet Co<sub>2</sub>FeO<sub>2</sub>BO<sub>3</sub>, a prominent example of lanthanide-free magnets, was the subject of element-selective studies using X-ray magnetic circular dichroism (XMCD) observations at the <i>L</i>- and <i>K</i>- X-ray absorption edges. Research findings indicate that the distinct magnetic characteristics of Co<sub>2</sub>FeO<sub>2</sub>BO<sub>3</sub>, namely its remarkable high coercivity (which surpasses 7 Tesla at low temperatures), originate from an atypical arrangement of magnetic ions in the crystal structure (sp.gr. <i>Pbam</i>). The antiferromagnetic nature of the Co<sup>2+</sup>-O-Fe<sup>3+</sup> exchange interaction was confirmed by identifying the spin and orbital contributions to the total magnetization from Co (m<sub>L</sub> = 0.27 ± 0.1 μ<sub>B</sub>/ion and m<sup>eff</sup><sub>S</sub> = 0.53 ± 0.1 μ<sub>B</sub>/ion) and Fe (m<sub>L</sub> = 0.05 ± 0.1 μ<sub>B</sub>/ion and m<sup>eff</sup><sub>S</sub> = 0.80 ± 0.1 μ<sub>B</sub>/ion) ions through element-selective XMCD analysis. Additionally, the research explicitly revealed that the strong magnetic anisotropy is a result of the significant unquenched orbital magnetic moment of Co, a feature that is also present in the related compound Co<sub>3</sub>O<sub>2</sub>BO<sub>3</sub>. A complex magnetic structure in Co<sub>2</sub>FeO<sub>2</sub>BO<sub>3</sub>, with infinite Co²⁺O<sub>6</sub> layers in the <b>bc</b>-plane and strong antiferromagnetic coupling through Fe<sup>3</sup>⁺ ions, is suggested by element-selective hysteresis data, which revealed that Co²⁺ ions contribute both antiferromagnetic and ferromagnetic components to the total magnetization. The findings underline the suitability of Co<sub>2</sub>FeO<sub>2</sub>BO<sub>3</sub> for applications in extreme environments, such as low temperatures and high magnetic fields, where its unique magnetic topology and anisotropy can be harnessed for advanced technologies, including materials for space exploration and quantum devices. This XMCD study opens the door to the production of novel high-coercivity, lanthanide-free magnetic materials by showing that targeted substitution at specific crystallographic sites can significantly enhance the magnetic properties of such materials.https://www.mdpi.com/2304-6740/13/1/24magnetismcoercive fieldelement-specificityorbital-specificitycharge ordering
spellingShingle Mikhail S. Platunov
High-Coercivity Ferrimagnet Co₂FeO₂BO₃: XMCD Insights into Charge-Ordering and Cation Distribution
Inorganics
magnetism
coercive field
element-specificity
orbital-specificity
charge ordering
title High-Coercivity Ferrimagnet Co₂FeO₂BO₃: XMCD Insights into Charge-Ordering and Cation Distribution
title_full High-Coercivity Ferrimagnet Co₂FeO₂BO₃: XMCD Insights into Charge-Ordering and Cation Distribution
title_fullStr High-Coercivity Ferrimagnet Co₂FeO₂BO₃: XMCD Insights into Charge-Ordering and Cation Distribution
title_full_unstemmed High-Coercivity Ferrimagnet Co₂FeO₂BO₃: XMCD Insights into Charge-Ordering and Cation Distribution
title_short High-Coercivity Ferrimagnet Co₂FeO₂BO₃: XMCD Insights into Charge-Ordering and Cation Distribution
title_sort high coercivity ferrimagnet co₂feo₂bo₃ xmcd insights into charge ordering and cation distribution
topic magnetism
coercive field
element-specificity
orbital-specificity
charge ordering
url https://www.mdpi.com/2304-6740/13/1/24
work_keys_str_mv AT mikhailsplatunov highcoercivityferrimagnetco2feo2bo3xmcdinsightsintochargeorderingandcationdistribution