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Quantum magnetisms in uniform triangular lattices Li(2)AMo(3)O(8) (A = In, Sc)
Molecular based spin-1/2 triangular lattice systems such as LiZn(2)Mo(3)O(8) have attracted research interest. Distortions, defects, and intersite disorder are suppressed in such molecular-based magnets, and intrinsic geometrical frustration gives rise to unconventional and unexpected ground states....
Autores principales: | , , , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2019
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6372599/ https://www.ncbi.nlm.nih.gov/pubmed/30755692 http://dx.doi.org/10.1038/s41598-018-36123-7 |
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author | Iida, Kazuki Yoshida, Hiroyuki Okabe, Hirotaka Katayama, Naoyuki Ishii, Yuto Koda, Akihiro Inamura, Yasuhiro Murai, Naoki Ishikado, Motoyuki Kadono, Ryosuke Kajimoto, Ryoichi |
author_facet | Iida, Kazuki Yoshida, Hiroyuki Okabe, Hirotaka Katayama, Naoyuki Ishii, Yuto Koda, Akihiro Inamura, Yasuhiro Murai, Naoki Ishikado, Motoyuki Kadono, Ryosuke Kajimoto, Ryoichi |
author_sort | Iida, Kazuki |
collection | PubMed |
description | Molecular based spin-1/2 triangular lattice systems such as LiZn(2)Mo(3)O(8) have attracted research interest. Distortions, defects, and intersite disorder are suppressed in such molecular-based magnets, and intrinsic geometrical frustration gives rise to unconventional and unexpected ground states. Li(2)AMo(3)O(8) (A = In or Sc) is such a compound where spin-1/2 Mo(3)O(13) clusters in place of Mo ions form the uniform triangular lattice. Their ground states are different according to the A site. Li(2)InMo(3)O(8) undergoes conventional 120° long-range magnetic order below T(N) = 12 K whereas isomorphic Li(2)ScMo(3)O(8) exhibits no long-range magnetic order down to 0.5 K. Here, we report exotic magnetisms in Li(2)InMo(3)O(8) and Li(2)ScMo(3)O(8) investigated by muon spin rotation (μSR) and inelastic neutron scattering (INS) spectroscopies using polycrystalline samples. Li(2)InMo(3)O(8) and Li(2)ScMo(3)O(8) show completely different behaviors observed in both μSR and INS measurements, representing their different ground states. Li(2)InMo(3)O(8) exhibits spin wave excitation which is quantitatively described by the nearest neighbor anisotropic Heisenberg model based on the 120° spin structure. In contrast, Li(2)ScMo(3)O(8) undergoes short-range magnetic order below 4 K with quantum-spin-liquid-like magnetic fluctuations down to the base temperature. Origin of the different ground states is discussed in terms of anisotropies of crystal structures and magnetic interactions. |
format | Online Article Text |
id | pubmed-6372599 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2019 |
publisher | Nature Publishing Group UK |
record_format | MEDLINE/PubMed |
spelling | pubmed-63725992019-02-19 Quantum magnetisms in uniform triangular lattices Li(2)AMo(3)O(8) (A = In, Sc) Iida, Kazuki Yoshida, Hiroyuki Okabe, Hirotaka Katayama, Naoyuki Ishii, Yuto Koda, Akihiro Inamura, Yasuhiro Murai, Naoki Ishikado, Motoyuki Kadono, Ryosuke Kajimoto, Ryoichi Sci Rep Article Molecular based spin-1/2 triangular lattice systems such as LiZn(2)Mo(3)O(8) have attracted research interest. Distortions, defects, and intersite disorder are suppressed in such molecular-based magnets, and intrinsic geometrical frustration gives rise to unconventional and unexpected ground states. Li(2)AMo(3)O(8) (A = In or Sc) is such a compound where spin-1/2 Mo(3)O(13) clusters in place of Mo ions form the uniform triangular lattice. Their ground states are different according to the A site. Li(2)InMo(3)O(8) undergoes conventional 120° long-range magnetic order below T(N) = 12 K whereas isomorphic Li(2)ScMo(3)O(8) exhibits no long-range magnetic order down to 0.5 K. Here, we report exotic magnetisms in Li(2)InMo(3)O(8) and Li(2)ScMo(3)O(8) investigated by muon spin rotation (μSR) and inelastic neutron scattering (INS) spectroscopies using polycrystalline samples. Li(2)InMo(3)O(8) and Li(2)ScMo(3)O(8) show completely different behaviors observed in both μSR and INS measurements, representing their different ground states. Li(2)InMo(3)O(8) exhibits spin wave excitation which is quantitatively described by the nearest neighbor anisotropic Heisenberg model based on the 120° spin structure. In contrast, Li(2)ScMo(3)O(8) undergoes short-range magnetic order below 4 K with quantum-spin-liquid-like magnetic fluctuations down to the base temperature. Origin of the different ground states is discussed in terms of anisotropies of crystal structures and magnetic interactions. Nature Publishing Group UK 2019-02-12 /pmc/articles/PMC6372599/ /pubmed/30755692 http://dx.doi.org/10.1038/s41598-018-36123-7 Text en © The Author(s) 2019 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 license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license 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 license, visit http://creativecommons.org/licenses/by/4.0/. |
spellingShingle | Article Iida, Kazuki Yoshida, Hiroyuki Okabe, Hirotaka Katayama, Naoyuki Ishii, Yuto Koda, Akihiro Inamura, Yasuhiro Murai, Naoki Ishikado, Motoyuki Kadono, Ryosuke Kajimoto, Ryoichi Quantum magnetisms in uniform triangular lattices Li(2)AMo(3)O(8) (A = In, Sc) |
title | Quantum magnetisms in uniform triangular lattices Li(2)AMo(3)O(8) (A = In, Sc) |
title_full | Quantum magnetisms in uniform triangular lattices Li(2)AMo(3)O(8) (A = In, Sc) |
title_fullStr | Quantum magnetisms in uniform triangular lattices Li(2)AMo(3)O(8) (A = In, Sc) |
title_full_unstemmed | Quantum magnetisms in uniform triangular lattices Li(2)AMo(3)O(8) (A = In, Sc) |
title_short | Quantum magnetisms in uniform triangular lattices Li(2)AMo(3)O(8) (A = In, Sc) |
title_sort | quantum magnetisms in uniform triangular lattices li(2)amo(3)o(8) (a = in, sc) |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6372599/ https://www.ncbi.nlm.nih.gov/pubmed/30755692 http://dx.doi.org/10.1038/s41598-018-36123-7 |
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