Hung-Cheng Wu, Takuya Aoyama, Daisuke Morikawa, Daisuke Okuyama, Kazuhiro Nawa, Wei-Tin Chen, Chan-Hung Lu, Tsung-Wen Yen, Shin-Ming Huang, Stuart Calder, Shuki Torii, Kenya Ohgushi, Masami Terauchi, Taku J. Sato
{"title":"Observation of Thermally Induced Piezomagnetic Switching in Cu2OSeO3 Polymorph Synthesized under High-Pressure","authors":"Hung-Cheng Wu, Takuya Aoyama, Daisuke Morikawa, Daisuke Okuyama, Kazuhiro Nawa, Wei-Tin Chen, Chan-Hung Lu, Tsung-Wen Yen, Shin-Ming Huang, Stuart Calder, Shuki Torii, Kenya Ohgushi, Masami Terauchi, Taku J. Sato","doi":"10.1002/apxr.202400054","DOIUrl":null,"url":null,"abstract":"<p>A polymorph of Cu<sub>2</sub>OSeO<sub>3</sub> with the distorted kagome lattice is successfully obtained using the high-pressure synthesis technique (Cu<sub>2</sub>OSeO<sub>3</sub>-HP). The structural analysis using X-ray and neutron powder diffraction suggests that the tetrahedral Cu<sup>2+</sup> clusters [similar to those in Cu<sub>2</sub>OSeO<sub>3</sub> ambient-pressure phase (Cu<sub>2</sub>OSeO<sub>3</sub>-AP)] exist in Cu<sub>2</sub>OSeO<sub>3</sub>-HP but with three symmetry inequivalent sites. No structural change is observed between 1.5 K and the room temperature. The complex magnetic H-<i>T</i> phase diagram is established based on the temperature- and field-dependent magnetization data, indicating two distinct antiferromagnetic phases at low and intermediate temperatures, in addition to the higher-temperature spin-glass-like phase. The low temperature phase is identified by neutron powder diffraction refinements as a canted noncollinear antiferromagnetic order with a weak ferromagnetic component along the <i>b</i>-axis. Size of the refined ordered moment is ≈1.00(4) µ<sub>B</sub> in Cu<sub>2</sub>OSeO<sub>3</sub>-HP, indicating a large enhancement compared to that of Cu<sub>2</sub>OSeO<sub>3</sub>-AP (≈0.61 µ<sub>B</sub>). By applying a uniaxial stress, finite enhancement of weak ferromagnetic component in the noncollinear antiferromagnetic phase in Cu<sub>2</sub>OSeO<sub>3</sub>-HP is observed, which is the clear evidence of the piezomagnetic effect. Interestingly, the sign of the induced magnetization changes on heating from the low-temperature to the intermediate-temperature phases, indicating a novel piezomagnetic switching effect in this compound.</p>","PeriodicalId":100035,"journal":{"name":"Advanced Physics Research","volume":"3 11","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-08-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1002/apxr.202400054","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Advanced Physics Research","FirstCategoryId":"1085","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1002/apxr.202400054","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
A polymorph of Cu2OSeO3 with the distorted kagome lattice is successfully obtained using the high-pressure synthesis technique (Cu2OSeO3-HP). The structural analysis using X-ray and neutron powder diffraction suggests that the tetrahedral Cu2+ clusters [similar to those in Cu2OSeO3 ambient-pressure phase (Cu2OSeO3-AP)] exist in Cu2OSeO3-HP but with three symmetry inequivalent sites. No structural change is observed between 1.5 K and the room temperature. The complex magnetic H-T phase diagram is established based on the temperature- and field-dependent magnetization data, indicating two distinct antiferromagnetic phases at low and intermediate temperatures, in addition to the higher-temperature spin-glass-like phase. The low temperature phase is identified by neutron powder diffraction refinements as a canted noncollinear antiferromagnetic order with a weak ferromagnetic component along the b-axis. Size of the refined ordered moment is ≈1.00(4) µB in Cu2OSeO3-HP, indicating a large enhancement compared to that of Cu2OSeO3-AP (≈0.61 µB). By applying a uniaxial stress, finite enhancement of weak ferromagnetic component in the noncollinear antiferromagnetic phase in Cu2OSeO3-HP is observed, which is the clear evidence of the piezomagnetic effect. Interestingly, the sign of the induced magnetization changes on heating from the low-temperature to the intermediate-temperature phases, indicating a novel piezomagnetic switching effect in this compound.