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Magnetic phase diagram of the solid solution LaMn(2)(Ge(1−x)Si(x))(2) (0 ≤ x ≤ 1) unraveled by powder neutron diffraction
The structural and magnetic properties of the ThCr(2)Si(2)-type solid solution LaMn(2)(Ge(1−x)Si(x))(2) (x = 0.0 to 1.0) have been investigated employing a combination of X-ray diffraction, magnetization and neutron diffraction measurements, which allowed establishing a magnetic composition-temperat...
Autores principales: | , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
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Nature Publishing Group UK
2022
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9166718/ https://www.ncbi.nlm.nih.gov/pubmed/35665754 http://dx.doi.org/10.1038/s41598-022-12549-y |
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author | Siebeneichler, Stefanie Ovchinnikov, Alexander Bosch-Santos, Brianna Cabrera-Pasca, Gabriel A. Flacau, Roxana Huang, Qingzhen Carbonari, Artur W. Ryan, Dominic Mudring, Anja-Verena |
author_facet | Siebeneichler, Stefanie Ovchinnikov, Alexander Bosch-Santos, Brianna Cabrera-Pasca, Gabriel A. Flacau, Roxana Huang, Qingzhen Carbonari, Artur W. Ryan, Dominic Mudring, Anja-Verena |
author_sort | Siebeneichler, Stefanie |
collection | PubMed |
description | The structural and magnetic properties of the ThCr(2)Si(2)-type solid solution LaMn(2)(Ge(1−x)Si(x))(2) (x = 0.0 to 1.0) have been investigated employing a combination of X-ray diffraction, magnetization and neutron diffraction measurements, which allowed establishing a magnetic composition-temperature phase diagram. Substitution of Ge by Si leads to a compression of the unit cell, which affects the magnetic exchange interactions. In particular, the magnetic structure of LaMn(2)(Ge(1−x)Si(x))(2) is strongly affected by the unit cell parameter c, which is related to the distance between adjacent Mn layers. Commensurate antiferromagnetic layers and a canted ferromagnetic structure dominate the Si-rich part of the solid solution, whilst an incommensurate antiferromagnetic flat spiral and a conical magnetic structure are observed in the Si-poor part. |
format | Online Article Text |
id | pubmed-9166718 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2022 |
publisher | Nature Publishing Group UK |
record_format | MEDLINE/PubMed |
spelling | pubmed-91667182022-06-05 Magnetic phase diagram of the solid solution LaMn(2)(Ge(1−x)Si(x))(2) (0 ≤ x ≤ 1) unraveled by powder neutron diffraction Siebeneichler, Stefanie Ovchinnikov, Alexander Bosch-Santos, Brianna Cabrera-Pasca, Gabriel A. Flacau, Roxana Huang, Qingzhen Carbonari, Artur W. Ryan, Dominic Mudring, Anja-Verena Sci Rep Article The structural and magnetic properties of the ThCr(2)Si(2)-type solid solution LaMn(2)(Ge(1−x)Si(x))(2) (x = 0.0 to 1.0) have been investigated employing a combination of X-ray diffraction, magnetization and neutron diffraction measurements, which allowed establishing a magnetic composition-temperature phase diagram. Substitution of Ge by Si leads to a compression of the unit cell, which affects the magnetic exchange interactions. In particular, the magnetic structure of LaMn(2)(Ge(1−x)Si(x))(2) is strongly affected by the unit cell parameter c, which is related to the distance between adjacent Mn layers. Commensurate antiferromagnetic layers and a canted ferromagnetic structure dominate the Si-rich part of the solid solution, whilst an incommensurate antiferromagnetic flat spiral and a conical magnetic structure are observed in the Si-poor part. Nature Publishing Group UK 2022-06-03 /pmc/articles/PMC9166718/ /pubmed/35665754 http://dx.doi.org/10.1038/s41598-022-12549-y Text en © The Author(s) 2022 https://creativecommons.org/licenses/by/4.0/Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article's Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article's Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit http://creativecommons.org/licenses/by/4.0/ (https://creativecommons.org/licenses/by/4.0/) . |
spellingShingle | Article Siebeneichler, Stefanie Ovchinnikov, Alexander Bosch-Santos, Brianna Cabrera-Pasca, Gabriel A. Flacau, Roxana Huang, Qingzhen Carbonari, Artur W. Ryan, Dominic Mudring, Anja-Verena Magnetic phase diagram of the solid solution LaMn(2)(Ge(1−x)Si(x))(2) (0 ≤ x ≤ 1) unraveled by powder neutron diffraction |
title | Magnetic phase diagram of the solid solution LaMn(2)(Ge(1−x)Si(x))(2) (0 ≤ x ≤ 1) unraveled by powder neutron diffraction |
title_full | Magnetic phase diagram of the solid solution LaMn(2)(Ge(1−x)Si(x))(2) (0 ≤ x ≤ 1) unraveled by powder neutron diffraction |
title_fullStr | Magnetic phase diagram of the solid solution LaMn(2)(Ge(1−x)Si(x))(2) (0 ≤ x ≤ 1) unraveled by powder neutron diffraction |
title_full_unstemmed | Magnetic phase diagram of the solid solution LaMn(2)(Ge(1−x)Si(x))(2) (0 ≤ x ≤ 1) unraveled by powder neutron diffraction |
title_short | Magnetic phase diagram of the solid solution LaMn(2)(Ge(1−x)Si(x))(2) (0 ≤ x ≤ 1) unraveled by powder neutron diffraction |
title_sort | magnetic phase diagram of the solid solution lamn(2)(ge(1−x)si(x))(2) (0 ≤ x ≤ 1) unraveled by powder neutron diffraction |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9166718/ https://www.ncbi.nlm.nih.gov/pubmed/35665754 http://dx.doi.org/10.1038/s41598-022-12549-y |
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