A B-site ordered double perovskite oxide CdCrSbO was synthesized under high-pressure and high-temperature conditions. The compound crystallizes to a monoclinic structure with a space group of 2/. The charge configuration is confirmed to be that of Cd/Cr/Sb.
View Article and Find Full Text PDFA transition-metal oxide of PbCuMnO was prepared at 1523 K and 10 GPa. An A-site-ordered quadruple perovskite structure with the space group 3̅ is assigned for this compound. Based on bond-valence-sum calculations and X-ray absorption spectroscopy, the charge combination is determined to be PbCuMnO.
View Article and Find Full Text PDFThe development of magnetocaloric materials with a significantly enhanced volumetric cooling capability is highly desirable for the application of adiabatic demagnetization refrigerators in confined spatial environments. Here, the thermodynamic characteristics of a magnetically frustrated spin-7/2 Gd[SiO]O is presented, which exhibits strongly correlated spin disorder below ≈1.5 K.
View Article and Find Full Text PDFAn AA'BB'O-type quadruple perovskite oxide of CaCuCrReO was synthesized at 18 GPa and 1373 K. Both an A- and B-site ordered quadruple perovskite crystal structure was observed, with the space group -3. The valence states are verified to be CaCuCrReO by bond valence sum calculations and synchrotron X-ray absorption spectroscopy.
View Article and Find Full Text PDFAn AA'BO-type A-site-ordered quadruple perovskite oxide AgMnO was prepared by high-pressure and high-temperature methods. At room temperature, the compound crystallizes into a cubic 3̅ symmetry with a charge distribution of AgMnMnO. With the temperature decreasing to ≈ 180 K, the compound undergoes a structural phase transition toward a monoclinic 2/ symmetry, giving rise to a B-site charge- and orbital-ordered AgMnMnMnO phase.
View Article and Find Full Text PDFCaCuMnTeO was synthesized using high-temperature and high-pressure conditions. The compound possesses an A- and B site ordered quadruple perovskite structure in 3̅ symmetry with the charge combination of CaCuMnTeO. A ferrimagnetic phase transition originating from the antiferromagnetic interaction between A' site Cu and B site Mn ions is found to occur at ≈ 100 K.
View Article and Find Full Text PDFMaterials with negative thermal expansion (NTE) attract significant research attention owing to their unique physical properties and promising applications. Although ferroelectric phase transitions leading to NTE are widely investigated, information on antiferroelectricity-induced NTE remains limited. In this study, single-crystal and polycrystalline Pb CoMoO samples are prepared at high pressure and temperature conditions.
View Article and Find Full Text PDFJ Phys Condens Matter
April 2023
The concurrent presence of large electric polarization and strong magnetoelectric coupling is quite desirable for potential applications of multiferroics. In this paper, we report the growth of CdMnOsingle crystals by flux method under a high pressure of 8 GPa for the first time. An antiferromagnetic (AFM) order with a polar magnetic point group is found to occur at the onset temperature of= 88 K (AFM1 phase).
View Article and Find Full Text PDFSearching for working refrigerant materials is the key element in the design of magnetic cooling devices. Herein, we report on the thermodynamic and magnetocaloric parameters of an phase oxyorthosilicate, GdSiO, by field-dependent static magnetization and specific heat measurements. An overall correlation strength of || ≈ 3.
View Article and Find Full Text PDF2D room-temperature magnetic materials are of great importance in future spintronic devices while only very few are reported. Herein, a plasma-enhanced chemical vapor deposition approach is exploited to construct the 2D room-temperature magnetic MnGa -H single crystal with a thickness down to 2.2 nm.
View Article and Find Full Text PDFHalf metals, in which one spin channel is conducting while the other is insulating with an energy gap, are theoretically considered to comprise 100% spin-polarized conducting electrons, and thus have promising applications in high-efficiency magnetic sensors, computer memory, magnetic recording, and so on. However, for practical applications, a high Curie temperature combined with a wide spin energy gap and large magnetization is required. Realizing such a high-performance combination is a key challenge.
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