Mode-crystallography analysis and magnetic structures of SrLnFeRuO6 (Ln = La, Pr, Nd) disordered perovskites.

IF 1.9 3区 化学
E Iturbe-Zabalo, O Fabelo, M Gateshki, J M Igartua
{"title":"Mode-crystallography analysis and magnetic structures of SrLnFeRuO6 (Ln = La, Pr, Nd) disordered perovskites.","authors":"E Iturbe-Zabalo,&nbsp;O Fabelo,&nbsp;M Gateshki,&nbsp;J M Igartua","doi":"10.1107/S0108768112044217","DOIUrl":null,"url":null,"abstract":"<p><p>The crystal and magnetic structures of SrLnFeRuO(6) (Ln = La, Pr, Nd) double perovskites have been investigated. All compounds crystallize with an orthorhombic Pbnm structure at room temperature. These materials show complete chemical disorder of Fe and Ru cations for all compounds. The distortion of the structure, relative to the ideal cubic perovskite, has been decomposed into distortion modes. It has been found that the primary modes of the distortion are octahedral tilting modes: R(4)(+) and M(3)(+). The crystal structure of SrPrFeRuO(6) has been studied from room temperature up to 1200 K by neutron powder diffraction. There is a structural phase transition from orthorhombic (space group Pbnm) to trigonal (space group R3c) at T = 1075 K. According to group theory no second-order transition is possible between these symmetries. Magnetic ordering for all the compounds is described by the magnetic propagation vector (0,0,0). SrPrFeRuO(6) shows ferrimagnetic order below ca 475 K, while SrLaFeRuO(6) (below ca 450 K) and SrNdFeRuO(6) (below ca 430 K) exhibit canted-antiferromagnetic order. The magnetic moments at low temperatures are m(Fe/Ru) = 1.88 (3)μ(B) for SrLaFeRuO(6) (2 K), m(Pr) = 0.46 (4)μ(B) and m(Fe/Ru) = 2.24μ(B) for SrPrFeRuO(6) (2 K), and m(Fe/Ru) = 1.92μ(B) for SrNdFeRuO(6) (10 K).</p>","PeriodicalId":7107,"journal":{"name":"Acta Crystallographica Section B-structural Science","volume":"68 Pt 6","pages":"590-601"},"PeriodicalIF":1.9000,"publicationDate":"2012-12-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1107/S0108768112044217","citationCount":"5","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Acta Crystallographica Section B-structural Science","FirstCategoryId":"92","ListUrlMain":"https://doi.org/10.1107/S0108768112044217","RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"2012/11/16 0:00:00","PubModel":"Epub","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 5

Abstract

The crystal and magnetic structures of SrLnFeRuO(6) (Ln = La, Pr, Nd) double perovskites have been investigated. All compounds crystallize with an orthorhombic Pbnm structure at room temperature. These materials show complete chemical disorder of Fe and Ru cations for all compounds. The distortion of the structure, relative to the ideal cubic perovskite, has been decomposed into distortion modes. It has been found that the primary modes of the distortion are octahedral tilting modes: R(4)(+) and M(3)(+). The crystal structure of SrPrFeRuO(6) has been studied from room temperature up to 1200 K by neutron powder diffraction. There is a structural phase transition from orthorhombic (space group Pbnm) to trigonal (space group R3c) at T = 1075 K. According to group theory no second-order transition is possible between these symmetries. Magnetic ordering for all the compounds is described by the magnetic propagation vector (0,0,0). SrPrFeRuO(6) shows ferrimagnetic order below ca 475 K, while SrLaFeRuO(6) (below ca 450 K) and SrNdFeRuO(6) (below ca 430 K) exhibit canted-antiferromagnetic order. The magnetic moments at low temperatures are m(Fe/Ru) = 1.88 (3)μ(B) for SrLaFeRuO(6) (2 K), m(Pr) = 0.46 (4)μ(B) and m(Fe/Ru) = 2.24μ(B) for SrPrFeRuO(6) (2 K), and m(Fe/Ru) = 1.92μ(B) for SrNdFeRuO(6) (10 K).

SrLnFeRuO6 (Ln = La, Pr, Nd)无序钙钛矿的模式晶体学分析和磁性结构。
研究了SrLnFeRuO(6) (Ln = La, Pr, Nd)双钙钛矿的晶体结构和磁性结构。所有化合物在室温下结晶成正交的pnm结构。这些材料显示出所有化合物的铁和钌的完全化学无序性。相对于理想的立方钙钛矿,该结构的畸变被分解为不同的畸变模式。发现畸变的主要模式是八面体倾斜模式:R(4)(+)和M(3)(+)。用中子粉末衍射法研究了SrPrFeRuO(6)在室温至1200 K范围内的晶体结构。在T = 1075 K时,结构相变由正交(空间群Pbnm)向三角(空间群R3c)转变。根据群论,这些对称之间不可能有二阶跃迁。所有化合物的磁有序用磁传播向量(0,0,0)来描述。SrPrFeRuO(6)在ca 475 K以下表现为铁磁有序,而SrLaFeRuO(6) (ca 450 K以下)和SrNdFeRuO(6) (ca 430 K以下)表现为倾斜的反铁磁有序。SrLaFeRuO(6) (2 K)的磁矩为m(Fe/Ru) = 1.88 (3)μ(B), SrPrFeRuO(6) (2 K)的磁矩为m(Pr) = 0.46 (4)μ(B)和m(Fe/Ru) = 2.24μ(B), SrNdFeRuO(6) (10 K)的磁矩为m(Fe/Ru) = 1.92μ(B)。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
来源期刊
自引率
5.30%
发文量
0
审稿时长
6-12 weeks
期刊介绍: Acta Crystallographica Section B: Structural Science, Crystal Engineering and Materials publishes scientific articles related to the structural science of compounds and materials in the widest sense. Knowledge of the arrangements of atoms, including their temporal variations and dependencies on temperature and pressure, is often the key to understanding physical and chemical phenomena and is crucial for the design of new materials and supramolecular devices. Acta Crystallographica B is the forum for the publication of such contributions. Scientific developments based on experimental studies as well as those based on theoretical approaches, including crystal-structure prediction, structure-property relations and the use of databases of crystal structures, are published.
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术官方微信