Observation of Thermally Induced Piezomagnetic Switching in Cu2OSeO3 Polymorph Synthesized under High‐Pressure

Author:

Wu Hung‐Cheng12ORCID,Aoyama Takuya3,Morikawa Daisuke1,Okuyama Daisuke1,Nawa Kazuhiro1,Chen Wei‐Tin45,Lu Chan‐Hung2,Yen Tsung‐Wen2,Huang Shin‐Ming2,Calder Stuart6,Torii Shuki7,Ohgushi Kenya3,Terauchi Masami1,Sato Taku J.1

Affiliation:

1. Institute of Multidisciplinary Research for Advanced Materials Tohoku University Sendai 980‐8577 Japan

2. Department of Physics National Sun Yat‐sen University Kaohsiung 80424 Taiwan

3. Department of Physics Graduate School of Science Tohoku University Sendai 980‐8578 Japan

4. Center for Condensed Matter Sciences and Center of Atomic Initiative for New Materials National Taiwan University Taipei 10617 Taiwan

5. Taiwan Consortium of Emergent Crystalline Materials National Science and Technology Council Taipei 10622 Taiwan

6. Neutron Scattering Division Oak Ridge National Laboratory Oak Ridge TN 37831 USA

7. Institute of Materials Structure Science High Energy Accelerator Research Organization 203‐1 Shirakata Tokai Ibaraki 319‐1106 Japan

Abstract

AbstractA 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.

Funder

National Science and Technology Council

Academia Sinica

Japan Society for the Promotion of Science London

Publisher

Wiley

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