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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...

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Autores principales: Xu, Zheying, Thakur, Pardeep K., Lee, Tien-Lin, Regoutz, Anna, Suard, Emmanuelle, Puente-Orench, Inés, Hayward, Michael A.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2022
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.
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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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