<HashMap><database>biostudies-literature</database><scores/><additional><submitter>Iida K</submitter><funding>NIEHS NIH HHS</funding><pagination>1826</pagination><full_dataset_link>https://www.ebi.ac.uk/biostudies/studies/S-EPMC6372599</full_dataset_link><repository>biostudies-literature</repository><omics_type>Unknown</omics_type><volume>9(1)</volume><pubmed_abstract>Molecular based spin-1/2 triangular lattice systems such as LiZn&lt;sub>2&lt;/sub>Mo&lt;sub>3&lt;/sub>O&lt;sub>8&lt;/sub> 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&lt;sub>2&lt;/sub>AMo&lt;sub>3&lt;/sub>O&lt;sub>8&lt;/sub> (A = In or Sc) is such a compound where spin-1/2 Mo&lt;sub>3&lt;/sub>O&lt;sub>13&lt;/sub> clusters in place of Mo ions form the uniform triangular lattice. Their ground states are different according to the A site. Li&lt;sub>2&lt;/sub>InMo&lt;sub>3&lt;/sub>O&lt;sub>8&lt;/sub> undergoes conventional 120° long-range magnetic order below T&lt;sub>N&lt;/sub> = 12 K whereas isomorphic Li&lt;sub>2&lt;/sub>ScMo&lt;sub>3&lt;/sub>O&lt;sub>8&lt;/sub> exhibits no long-range magnetic order down to 0.5 K. Here, we report exotic magnetisms in Li&lt;sub>2&lt;/sub>InMo&lt;sub>3&lt;/sub>O&lt;sub>8&lt;/sub> and Li&lt;sub>2&lt;/sub>ScMo&lt;sub>3&lt;/sub>O&lt;sub>8&lt;/sub> investigated by muon spin rotation (μSR) and inelastic neutron scattering (INS) spectroscopies using polycrystalline samples. Li&lt;sub>2&lt;/sub>InMo&lt;sub>3&lt;/sub>O&lt;sub>8&lt;/sub> and Li&lt;sub>2&lt;/sub>ScMo&lt;sub>3&lt;/sub>O&lt;sub>8&lt;/sub> show completely different behaviors observed in both μSR and INS measurements, representing their different ground states. Li&lt;sub>2&lt;/sub>InMo&lt;sub>3&lt;/sub>O&lt;sub>8&lt;/sub> exhibits spin wave excitation which is quantitatively described by the nearest neighbor anisotropic Heisenberg model based on the 120° spin structure. In contrast, Li&lt;sub>2&lt;/sub>ScMo&lt;sub>3&lt;/sub>O&lt;sub>8&lt;/sub> 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.</pubmed_abstract><journal>Scientific reports</journal><pubmed_title>Quantum magnetisms in uniform triangular lattices Li&lt;sub>2&lt;/sub>AMo&lt;sub>3&lt;/sub>O&lt;sub>8&lt;/sub> (A = In, Sc).</pubmed_title><pmcid>PMC6372599</pmcid><funding_grant_id>27399I0001</funding_grant_id><pubmed_authors>Iida K</pubmed_authors><pubmed_authors>Koda A</pubmed_authors><pubmed_authors>Katayama N</pubmed_authors><pubmed_authors>Okabe H</pubmed_authors><pubmed_authors>Ishii Y</pubmed_authors><pubmed_authors>Murai N</pubmed_authors><pubmed_authors>Yoshida H</pubmed_authors><pubmed_authors>Inamura Y</pubmed_authors><pubmed_authors>Kajimoto R</pubmed_authors><pubmed_authors>Ishikado M</pubmed_authors><pubmed_authors>Kadono R</pubmed_authors></additional><is_claimable>false</is_claimable><name>Quantum magnetisms in uniform triangular lattices Li&lt;sub>2&lt;/sub>AMo&lt;sub>3&lt;/sub>O&lt;sub>8&lt;/sub> (A = In, Sc).</name><description>Molecular based spin-1/2 triangular lattice systems such as LiZn&lt;sub>2&lt;/sub>Mo&lt;sub>3&lt;/sub>O&lt;sub>8&lt;/sub> 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&lt;sub>2&lt;/sub>AMo&lt;sub>3&lt;/sub>O&lt;sub>8&lt;/sub> (A = In or Sc) is such a compound where spin-1/2 Mo&lt;sub>3&lt;/sub>O&lt;sub>13&lt;/sub> clusters in place of Mo ions form the uniform triangular lattice. Their ground states are different according to the A site. Li&lt;sub>2&lt;/sub>InMo&lt;sub>3&lt;/sub>O&lt;sub>8&lt;/sub> undergoes conventional 120° long-range magnetic order below T&lt;sub>N&lt;/sub> = 12 K whereas isomorphic Li&lt;sub>2&lt;/sub>ScMo&lt;sub>3&lt;/sub>O&lt;sub>8&lt;/sub> exhibits no long-range magnetic order down to 0.5 K. Here, we report exotic magnetisms in Li&lt;sub>2&lt;/sub>InMo&lt;sub>3&lt;/sub>O&lt;sub>8&lt;/sub> and Li&lt;sub>2&lt;/sub>ScMo&lt;sub>3&lt;/sub>O&lt;sub>8&lt;/sub> investigated by muon spin rotation (μSR) and inelastic neutron scattering (INS) spectroscopies using polycrystalline samples. Li&lt;sub>2&lt;/sub>InMo&lt;sub>3&lt;/sub>O&lt;sub>8&lt;/sub> and Li&lt;sub>2&lt;/sub>ScMo&lt;sub>3&lt;/sub>O&lt;sub>8&lt;/sub> show completely different behaviors observed in both μSR and INS measurements, representing their different ground states. Li&lt;sub>2&lt;/sub>InMo&lt;sub>3&lt;/sub>O&lt;sub>8&lt;/sub> exhibits spin wave excitation which is quantitatively described by the nearest neighbor anisotropic Heisenberg model based on the 120° spin structure. In contrast, Li&lt;sub>2&lt;/sub>ScMo&lt;sub>3&lt;/sub>O&lt;sub>8&lt;/sub> 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.</description><dates><release>2019-01-01T00:00:00Z</release><publication>2019 Feb</publication><modification>2024-11-11T19:38:38.567Z</modification><creation>2019-03-26T22:55:43Z</creation></dates><accession>S-EPMC6372599</accession><cross_references><pubmed>30755692</pubmed><doi>10.1038/s41598-018-36123-7</doi></cross_references></HashMap>