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Complex Magnetic Order in Topochemically Reduced Rh(I)/Rh(III) LaM(0.5)Rh(0.5)O(2.25) (M = Co, Ni) Phases
[Image: see text] Topochemical reduction of the cation-disordered perovskite oxides LaCo(0.5)Rh(0.5)O(3) and LaNi(0.5)Rh(0.5)O(3) with Zr yields the partially anion-vacancy ordered phases LaCo(0.5)Rh(0.5)O(2.25) and LaNi(0.5)Rh(0.5)O(2.25), respectively. Neutron diffraction and Hard X-ray photoelect...
Autores principales: | , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2022
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9533305/ https://www.ncbi.nlm.nih.gov/pubmed/36129165 http://dx.doi.org/10.1021/acs.inorgchem.2c02747 |
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author | Xu, Zheying Thakur, Pardeep K. Lee, Tien-Lin Regoutz, Anna Suard, Emmanuelle Puente-Orench, Inés Hayward, Michael A. |
author_facet | Xu, Zheying Thakur, Pardeep K. Lee, Tien-Lin Regoutz, Anna Suard, Emmanuelle Puente-Orench, Inés Hayward, Michael A. |
author_sort | Xu, Zheying |
collection | PubMed |
description | [Image: see text] Topochemical reduction of the cation-disordered perovskite oxides LaCo(0.5)Rh(0.5)O(3) and LaNi(0.5)Rh(0.5)O(3) with Zr yields the partially anion-vacancy ordered phases LaCo(0.5)Rh(0.5)O(2.25) and LaNi(0.5)Rh(0.5)O(2.25), respectively. Neutron diffraction and Hard X-ray photoelectron spectroscopy (HAXPES) measurements reveal that the anion-deficient phases contain Co(1+)/Ni(1+) and a 1:1 mixture of Rh(1+) and Rh(3+) cations within a disordered array of apex-linked MO(4) square-planar and MO(5) square-based pyramidal coordination sites. Neutron diffraction data indicate that LaCo(0.5)Rh(0.5)O(2.25) adopts a complex antiferromagnetic ground state, which is the sum of a C-type ordering (mM(5)(+)) of the xy-components of the Co spins and a G-type ordering (mΓ(1)(+)) of the z-components of the Co spins. On warming above 75 K, the magnitude of the mΓ(1)(+) component declines, attaining a zero value by 125 K, with the magnitude of the mM(5)(+) component remaining unchanged up to 175 K. This magnetic behavior is rationalized on the basis of the differing d-orbital fillings of the Co(1+) cations in MO(4) square-planar and MO(5) square-based pyramidal coordination sites. LaNi(0.5)Rh(0.5)O(2.25) shows no sign of long-range magnetic order at 2 K – behavior that can also be explained on the basis of the d-orbital occupation of the Ni(1+) centers. |
format | Online Article Text |
id | pubmed-9533305 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2022 |
publisher | American Chemical Society |
record_format | MEDLINE/PubMed |
spelling | pubmed-95333052022-10-06 Complex Magnetic Order in Topochemically Reduced Rh(I)/Rh(III) LaM(0.5)Rh(0.5)O(2.25) (M = Co, Ni) Phases Xu, Zheying Thakur, Pardeep K. Lee, Tien-Lin Regoutz, Anna Suard, Emmanuelle Puente-Orench, Inés Hayward, Michael A. Inorg Chem [Image: see text] Topochemical reduction of the cation-disordered perovskite oxides LaCo(0.5)Rh(0.5)O(3) and LaNi(0.5)Rh(0.5)O(3) with Zr yields the partially anion-vacancy ordered phases LaCo(0.5)Rh(0.5)O(2.25) and LaNi(0.5)Rh(0.5)O(2.25), respectively. Neutron diffraction and Hard X-ray photoelectron spectroscopy (HAXPES) measurements reveal that the anion-deficient phases contain Co(1+)/Ni(1+) and a 1:1 mixture of Rh(1+) and Rh(3+) cations within a disordered array of apex-linked MO(4) square-planar and MO(5) square-based pyramidal coordination sites. Neutron diffraction data indicate that LaCo(0.5)Rh(0.5)O(2.25) adopts a complex antiferromagnetic ground state, which is the sum of a C-type ordering (mM(5)(+)) of the xy-components of the Co spins and a G-type ordering (mΓ(1)(+)) of the z-components of the Co spins. On warming above 75 K, the magnitude of the mΓ(1)(+) component declines, attaining a zero value by 125 K, with the magnitude of the mM(5)(+) component remaining unchanged up to 175 K. This magnetic behavior is rationalized on the basis of the differing d-orbital fillings of the Co(1+) cations in MO(4) square-planar and MO(5) square-based pyramidal coordination sites. LaNi(0.5)Rh(0.5)O(2.25) shows no sign of long-range magnetic order at 2 K – behavior that can also be explained on the basis of the d-orbital occupation of the Ni(1+) centers. American Chemical Society 2022-09-21 2022-10-03 /pmc/articles/PMC9533305/ /pubmed/36129165 http://dx.doi.org/10.1021/acs.inorgchem.2c02747 Text en © 2022 The Authors. Published by 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 | Xu, Zheying Thakur, Pardeep K. Lee, Tien-Lin Regoutz, Anna Suard, Emmanuelle Puente-Orench, Inés Hayward, Michael A. Complex Magnetic Order in Topochemically Reduced Rh(I)/Rh(III) LaM(0.5)Rh(0.5)O(2.25) (M = Co, Ni) Phases |
title | Complex Magnetic
Order in Topochemically Reduced Rh(I)/Rh(III)
LaM(0.5)Rh(0.5)O(2.25) (M = Co, Ni) Phases |
title_full | Complex Magnetic
Order in Topochemically Reduced Rh(I)/Rh(III)
LaM(0.5)Rh(0.5)O(2.25) (M = Co, Ni) Phases |
title_fullStr | Complex Magnetic
Order in Topochemically Reduced Rh(I)/Rh(III)
LaM(0.5)Rh(0.5)O(2.25) (M = Co, Ni) Phases |
title_full_unstemmed | Complex Magnetic
Order in Topochemically Reduced Rh(I)/Rh(III)
LaM(0.5)Rh(0.5)O(2.25) (M = Co, Ni) Phases |
title_short | Complex Magnetic
Order in Topochemically Reduced Rh(I)/Rh(III)
LaM(0.5)Rh(0.5)O(2.25) (M = Co, Ni) Phases |
title_sort | complex magnetic
order in topochemically reduced rh(i)/rh(iii)
lam(0.5)rh(0.5)o(2.25) (m = co, ni) phases |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9533305/ https://www.ncbi.nlm.nih.gov/pubmed/36129165 http://dx.doi.org/10.1021/acs.inorgchem.2c02747 |
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