Pressure-induced charge orders and their postulated coupling to magnetism in hexagonal multiferroic LuFe2O4

  • Fengliang Liu
  • , Yiqing Hao
  • , Jinyang Ni
  • , Yongsheng Zhao
  • , Dongzhou Zhang
  • , Gilberto Fabbris
  • , Daniel Haskel
  • , Shaobo Cheng
  • , Xiaoshan Xu
  • , Lifeng Yin
  • , Hongjun Xiang
  • , Jun Zhao
  • , Xujie Lü
  • , Wenbin Wang
  • , Jian Shen
  • , Wenge Yang

Research output: Contribution to journalArticlepeer-review

5 Scopus citations

Abstract

Hexagonal LuFe2O4 is a promising charge order (CO) driven multiferroic material with high charge and spin-ordering temperatures. The coexisting charge and spin orders on Fe3+/Fe2+ sites result in magnetoelectric behaviors, but the coupling mechanism between the charge and spin orders remains elusive. Here, by tuning external pressure, we reveal three charge-ordered phases with suggested correlation to magnetic orders in LuFe2O4: (i) a centrosymmetric incommensurate three-dimensional CO with ferrimagnetism, (ii) a non-centrosymmetric incommensurate quasi-two-dimensional CO with ferrimagnetism, and (iii) a centrosymmetric commensurate CO with antiferromagnetism. Experimental in situ single-crystal X-ray diffraction and X-ray magnetic circular dichroism measurements combined with density functional theory calculations suggest that the charge density redistribution caused by pressure-induced compression in the frustrated double-layer [Fe2O4] cluster is responsible for the correlated spin-charge phase transitions. The pressure-enhanced effective Coulomb interactions among Fe-Fe bonds drive the frustrated (1/3, 1/3) CO to a less frustrated (1/4, 1/4) CO, which induces the ferrimagnetic to antiferromagnetic transition. Our results not only elucidate the coupling mechanism among charge, spin, and lattice degrees of freedom in LuFe2O4, but also provide a new way to tune the spin-charge orders in a highly controlled manner.

Original languageEnglish
Article number1
Journalnpj Quantum Materials
Volume8
Issue number1
DOIs
StatePublished - Dec 2023
Externally publishedYes

Funding

This work was supported by the National Natural Science Foundation of China (Grant Nos. U1930401, 12074071, 51772184, and 11991060) and the National Key Research Program of China (2016YFA0300702). We acknowledge Dr. Lili Zhang, Dr. Sheng Jiang, and Dr. Aiguo Li of 15U1 at SSRF and Dr. Changyong Park at HPCAT, APS, ANL for the technical support on the high-pressure XRD experiment. Gas loading by Sergey N. Tkachev is also acknowledged. HPCAT operations are supported by DOE-NNSA under Award No. DE-NA0001974 and DOE-BES under Award No. DE-FG02-99ER45775, with partial instrumentation funding by NSF. The SXD measurement was conducted at 13BM-C, APS, and ANL. 13BM-C operation is supported by COMPRES through the Partnership for Extreme Crystallography (PX2) project, under NSF Cooperative Agreement EAR-1661511, and by GSECARS under NSF EAR-1634415. The XMCD experiment was conducted at beamline 4ID-D, APS, and ANL. This research used resources from the Advanced Photon Source, a US Department of Energy (DOE) Office of Science User Facility operated for the DOE Office of Science by Argonne National Laboratory under Contract No. DE-AC02-06CH11357. This work was supported by the National Natural Science Foundation of China (Grant Nos. U1930401, 12074071, 51772184, and 11991060) and the National Key Research Program of China (2016YFA0300702). We acknowledge Dr. Lili Zhang, Dr. Sheng Jiang, and Dr. Aiguo Li of 15U1 at SSRF and Dr. Changyong Park at HPCAT, APS, ANL for the technical support on the high-pressure XRD experiment. Gas loading by Sergey N. Tkachev is also acknowledged. HPCAT operations are supported by DOE-NNSA under Award No. DE-NA0001974 and DOE-BES under Award No. DE-FG02-99ER45775, with partial instrumentation funding by NSF. The SXD measurement was conducted at 13BM-C, APS, and ANL. 13BM-C operation is supported by COMPRES through the Partnership for Extreme Crystallography (PX2) project, under NSF Cooperative Agreement EAR-1661511, and by GSECARS under NSF EAR-1634415. The XMCD experiment was conducted at beamline 4ID-D, APS, and ANL. This research used resources from the Advanced Photon Source, a US Department of Energy (DOE) Office of Science User Facility operated for the DOE Office of Science by Argonne National Laboratory under Contract No. DE-AC02-06CH11357.

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