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Wolff KK, Agrestini S, Tanaka A, Jansen M, Tjeng LH. Comparative Study of Potentially J
eff
= 0 Ground State Iridium(V) in SrLaNiIrO6
, SrLaMgIrO6
, and SrLaZnIrO6. Z Anorg Allg Chem 2017. [DOI: 10.1002/zaac.201700386] [Citation(s) in RCA: 16] [Impact Index Per Article: 2.0] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/10/2022]
Affiliation(s)
- Klaus K. Wolff
- Max Planck Institute for Chemical Physics of Solids; 01187 Dresden Germany
| | - Stefano Agrestini
- Max Planck Institute for Chemical Physics of Solids; 01187 Dresden Germany
| | - Arata Tanaka
- Department of Quantum Matter, AdSM; Hiroshima University; 739-8530 Higashi-Hiroshima Japan
| | - Martin Jansen
- Max Planck Institute for Chemical Physics of Solids; 01187 Dresden Germany
- Max Planck Institute for Solid State Research; 70569 Stuttgart Germany
| | - Liu Hao Tjeng
- Max Planck Institute for Chemical Physics of Solids; 01187 Dresden Germany
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Yuan Y, Feng HL, Ghimire MP, Matsushita Y, Tsujimoto Y, He J, Tanaka M, Katsuya Y, Yamaura K. High-pressure synthesis, crystal structures, and magnetic properties of 5d double-perovskite oxides Ca2MgOsO6 and Sr2MgOsO6. Inorg Chem 2015; 54:3422-31. [PMID: 25751088 DOI: 10.1021/ic503086a] [Citation(s) in RCA: 53] [Impact Index Per Article: 5.3] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/28/2022]
Abstract
Double-perovskite oxides Ca2MgOsO6 and Sr2MgOsO6 have been synthesized under high-pressure and high-temperature conditions (6 GPa and 1500 °C). Their crystal structures and magnetic properties were studied by a synchrotron X-ray diffraction experiment and by magnetic susceptibility, specific heat, isothermal magnetization, and electrical resistivity measurements. Ca2MgOsO6 and Sr2MgOsO6 crystallized in monoclinic (P21/n) and tetragonal (I4/m) double-perovskite structures, respectively; the degree of order of the Os and Mg arrangement was 96% or higher. Although Ca2MgOsO6 and Sr2MgOsO6 are isoelectric, a magnetic-glass transition was observed for Ca2MgOsO6 at 19 K, while Sr2MgOsO6 showed an antiferromagnetic transition at 110 K. The antiferromagnetic-transition temperature is the highest in the family. A first-principles density functional approach revealed that Ca2MgOsO6 and Sr2MgOsO6 are likely to be antiferromagnetic Mott insulators in which the band gaps open, with Coulomb correlations of ∼1.8-3.0 eV. These compounds offer a better opportunity for the clarification of the basis of 5d magnetic sublattices, with regard to the possible use of perovskite-related oxides in multifunctional devices. The double-perovskite oxides Ca2MgOsO6 and Sr2MgOsO6 are likely to be Mott insulators with a magnetic-glass (MG) transition at ∼19 K and an antiferromagnetic (AFM) transition at ∼110 K, respectively. This AFM transition temperature is the highest among double-perovskite oxides containing single magnetic sublattices. Thus, these compounds offer valuable opportunities for studying the magnetic nature of 5d perovskite-related oxides, with regard to their possible use in multifunctional devices.
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Affiliation(s)
- Yahua Yuan
- †Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan.,‡Graduate School of Chemical Sciences and Engineering, Hokkaido University, North 10 West 8, Kita-ku, Sapporo, Hokkaido 060-0810, Japan
| | - Hai L Feng
- †Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan.,‡Graduate School of Chemical Sciences and Engineering, Hokkaido University, North 10 West 8, Kita-ku, Sapporo, Hokkaido 060-0810, Japan
| | | | - Yoshitaka Matsushita
- ∇Materials Analysis Station, National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan
| | - Yoshihiro Tsujimoto
- ⊥Materials Processing Unit, National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan
| | - Jianfeng He
- †Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan.,‡Graduate School of Chemical Sciences and Engineering, Hokkaido University, North 10 West 8, Kita-ku, Sapporo, Hokkaido 060-0810, Japan
| | - Masahiko Tanaka
- #Synchrotron X-ray Station at SPring-8, National Institute for Materials Science, Kohto 1-1-1, Sayo-cho, Hyogo 679-5148, Japan
| | - Yoshio Katsuya
- #Synchrotron X-ray Station at SPring-8, National Institute for Materials Science, Kohto 1-1-1, Sayo-cho, Hyogo 679-5148, Japan
| | - Kazunari Yamaura
- †Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan.,‡Graduate School of Chemical Sciences and Engineering, Hokkaido University, North 10 West 8, Kita-ku, Sapporo, Hokkaido 060-0810, Japan
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Orayech B, Faik A, López GA, Fabelo O, Igartua JM. Mode-crystallography analysis of the crystal structures and the low- and high-temperature phase transitions in Na0.5K0.5NbO3. J Appl Crystallogr 2015. [DOI: 10.1107/s1600576715000941] [Citation(s) in RCA: 35] [Impact Index Per Article: 3.5] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/10/2022] Open
Abstract
Na0.5K0.5NbO3has been synthesized by the conventional solid-state reaction process. The crystal structures and phase transitions, at low and high temperature, determined from the Rietveld refinements of X-ray and neutron powder diffraction data are reported. The structure evolution of Na0.5K0.5NbO3in the temperature range from 2 to 875 K shows the presence of three phase transitions. The first one, at ∼135 K, is discontinuous from the rhombohedralR3c(No. 161) space group to the room-temperature orthorhombicAmm2 (No. 38) space group; the second is discontinuous from the orthorhombic to the tetragonalP4mmspace group (No. 99) at ∼465 K, and the third is continuous from the tetragonal to the cubic Pm\overline{3}m space group (No. 221) at ∼700 K. The obtained phase-transition sequence isR3c→Amm2 →P4mm→Pm\overline{3}m. No previous studies at low temperature have been carried out on the material with composition Na0.5K0.5NbO3. In the course of the determination of the three experimentally found phases, a novel method of refinement is presented. This is a step forward in the use of the symmetry-adapted modes as degrees of freedom in the refinement process: the parameterization of a direction in the internal space of the, in this case, sole irreducible representation, GM4−, responsible for the symmetry breaking from the parent cubic space group to the polar distorted low-symmetry phases. Eventually, this procedure enables the calculation of the spontaneous polarization.
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Orayech B, Urcelay-Olabarria I, López GA, Fabelo O, Faik A, Igartua JM. Synthesis, structural, magnetic and phase-transition studies of the ferromagnetic La2CoMnO6 double perovskite by symmetry-adapted modes. Dalton Trans 2015; 44:13867-80. [DOI: 10.1039/c5dt01532d] [Citation(s) in RCA: 24] [Impact Index Per Article: 2.4] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/21/2022]
Abstract
A powdered La2CoMnO6 double perovskite was synthesized by the solid-state reaction method, and its crystal structure and phase-transitions were investigated by (Mode Crystallography) Rietveld analysis using X-ray and neutron diffraction data. Three indistinguishable ferromagnetic models with the space groups P21/n and P2′1/n′ are proposed.
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Affiliation(s)
- B. Orayech
- Departamento de Física de la Materia Condensada
- Universidad del País Vasco
- Bilbao 48080
- Spain
| | - I. Urcelay-Olabarria
- Departamento de Física de la Materia Condensada
- Universidad del País Vasco
- Bilbao 48080
- Spain
- BCMaterials
| | - G. A. López
- Fisika Aplikatua II Saila
- Zientzia eta Teknologia Fakultatea
- Euskal Herriko Unibertsitatea
- Bilbao 48080
- Spain
| | - O. Fabelo
- Institut Laue-Langevin (ILL)
- 38042 Grenoble Cedex 9
- France
| | - A. Faik
- CICenergigune
- 01510 Miñano
- Spain
| | - J. M. Igartua
- Fisika Aplikatua II Saila
- Zientzia eta Teknologia Fakultatea
- Euskal Herriko Unibertsitatea
- Bilbao 48080
- Spain
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