La和Ru掺杂Sr2IrO4的磁性和电子行为。

IF 2.3 4区 物理与天体物理 Q3 PHYSICS, CONDENSED MATTER
B Dundi Sri Chandana, Jeetendra Kumar Tiwari, K Saranya, Arpita Rana, G Senthil Murugan, Namasivayam Dhenadhayalan, Kwang-Yong Choi, K C Sekhar, P D Babu, Raman Sankar, I Panneer Muthuselvam
{"title":"La和Ru掺杂Sr2IrO4的磁性和电子行为。","authors":"B Dundi Sri Chandana, Jeetendra Kumar Tiwari, K Saranya, Arpita Rana, G Senthil Murugan, Namasivayam Dhenadhayalan, Kwang-Yong Choi, K C Sekhar, P D Babu, Raman Sankar, I Panneer Muthuselvam","doi":"10.1088/1361-648X/ada47a","DOIUrl":null,"url":null,"abstract":"<p><p>We report a detailed experimental study of the structural, magnetic and electrical properties of La and Ru doped (Sr<sub>1-<i>x</i></sub>La<i><sub>x</sub></i>)<sub>2</sub>Ir<sub>1-<i>x</i></sub>Ru<i><sub>x</sub></i>O<sub>4</sub>(<i>x</i>= 0.05, 0.15). X-ray diffraction analysis reveals that both samples crystallize in a tetragonal structure with a space group<i>I</i>4<sub>1</sub>/<i>acd</i>without impurities. Substitution with La and Ru leads to an increase in the lattice parameter<i>a</i>and a decrease in<i>c</i>. With increasing doping concentration, the Ir-O-Ir bond angle increases while the Ir-O bond length decreases. X-ray photoelectron spectroscopy (XPS) shows that Ir has Ir<sup>3+</sup>(5<i>d</i><sup>6</sup>) and Ir<sup>4+</sup>(5<i>d</i><sup>5</sup>) charge states, where the Ir<sup>4+</sup>charge state decreases with an increase in doping concentration. The<i>dc</i>magnetic susceptibility<i>χ</i>(<i>T</i>) of<i>x</i>= 0.05 reveals a transition from paramagnetic to weak ferromagnetic (wFM) at<i>T</i><sub>C</sub>∼ 229 K, arising from the canted antiferromagnetic (AFM) spin arrangement. The magnetic ordering temperature<i>T</i><sub>C</sub>remains unaltered for higher doping, whereas the magnetic moment is significantly reduced. The analysis of real and imaginary components of<i>ac</i>susceptibility data, based on conventional critical slow model, frequency shift per decade and Vogel-Fulcher law, unanimously evidences the existence of reentrant spin-glass behavior (RSG), i.e. the coexistence of weak ferromagnetism and spin glass phases for the lowest doping of<i>x</i>= 0.05. On the other hand, for higher doping (<i>x</i>= 0.15) of hole and electron, the RSG phase vanishes, leaving only the wFM phase at the same temperature as observed in<i>x</i>= 0.05. This suggests the higher doping of La and Ru does not affect the magnetic order, but removes the disorder between FM and AFM phases. The electrical resistivity (<i>ρ</i>) measurement analysis reveals that both the samples show semiconducting/insulating behavior across the temperature range. The<i>ρ</i>of the<i>x</i>= 0.05 sample is lower than that of pure sample Sr<sub>2</sub>IrO<sub>4</sub>(Bhatti<i>et al 2015 J. Phys.:Condens. Matter</i><b>27</b>016005), while<i>ρ</i>of<i>x</i>= 0.15 shows two orders of magnitude larger than the<i>x</i>= 0.05 sample at low temperatures. The conduction mechanism of both samples is described by the 2D Mott's variable-range hopping model. Our results demonstrate that co-doping of two cation sites generates intriguing, competing hopping and magnetic processes.</p>","PeriodicalId":16776,"journal":{"name":"Journal of Physics: Condensed Matter","volume":" ","pages":""},"PeriodicalIF":2.3000,"publicationDate":"2025-01-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Intriguing magnetic and electronic behaviors in La and Ru doped Sr<sub>2</sub>IrO<sub>4</sub>.\",\"authors\":\"B Dundi Sri Chandana, Jeetendra Kumar Tiwari, K Saranya, Arpita Rana, G Senthil Murugan, Namasivayam Dhenadhayalan, Kwang-Yong Choi, K C Sekhar, P D Babu, Raman Sankar, I Panneer Muthuselvam\",\"doi\":\"10.1088/1361-648X/ada47a\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p><p>We report a detailed experimental study of the structural, magnetic and electrical properties of La and Ru doped (Sr<sub>1-<i>x</i></sub>La<i><sub>x</sub></i>)<sub>2</sub>Ir<sub>1-<i>x</i></sub>Ru<i><sub>x</sub></i>O<sub>4</sub>(<i>x</i>= 0.05, 0.15). X-ray diffraction analysis reveals that both samples crystallize in a tetragonal structure with a space group<i>I</i>4<sub>1</sub>/<i>acd</i>without impurities. Substitution with La and Ru leads to an increase in the lattice parameter<i>a</i>and a decrease in<i>c</i>. With increasing doping concentration, the Ir-O-Ir bond angle increases while the Ir-O bond length decreases. X-ray photoelectron spectroscopy (XPS) shows that Ir has Ir<sup>3+</sup>(5<i>d</i><sup>6</sup>) and Ir<sup>4+</sup>(5<i>d</i><sup>5</sup>) charge states, where the Ir<sup>4+</sup>charge state decreases with an increase in doping concentration. The<i>dc</i>magnetic susceptibility<i>χ</i>(<i>T</i>) of<i>x</i>= 0.05 reveals a transition from paramagnetic to weak ferromagnetic (wFM) at<i>T</i><sub>C</sub>∼ 229 K, arising from the canted antiferromagnetic (AFM) spin arrangement. The magnetic ordering temperature<i>T</i><sub>C</sub>remains unaltered for higher doping, whereas the magnetic moment is significantly reduced. The analysis of real and imaginary components of<i>ac</i>susceptibility data, based on conventional critical slow model, frequency shift per decade and Vogel-Fulcher law, unanimously evidences the existence of reentrant spin-glass behavior (RSG), i.e. the coexistence of weak ferromagnetism and spin glass phases for the lowest doping of<i>x</i>= 0.05. On the other hand, for higher doping (<i>x</i>= 0.15) of hole and electron, the RSG phase vanishes, leaving only the wFM phase at the same temperature as observed in<i>x</i>= 0.05. This suggests the higher doping of La and Ru does not affect the magnetic order, but removes the disorder between FM and AFM phases. The electrical resistivity (<i>ρ</i>) measurement analysis reveals that both the samples show semiconducting/insulating behavior across the temperature range. The<i>ρ</i>of the<i>x</i>= 0.05 sample is lower than that of pure sample Sr<sub>2</sub>IrO<sub>4</sub>(Bhatti<i>et al 2015 J. Phys.:Condens. Matter</i><b>27</b>016005), while<i>ρ</i>of<i>x</i>= 0.15 shows two orders of magnitude larger than the<i>x</i>= 0.05 sample at low temperatures. The conduction mechanism of both samples is described by the 2D Mott's variable-range hopping model. Our results demonstrate that co-doping of two cation sites generates intriguing, competing hopping and magnetic processes.</p>\",\"PeriodicalId\":16776,\"journal\":{\"name\":\"Journal of Physics: Condensed Matter\",\"volume\":\" \",\"pages\":\"\"},\"PeriodicalIF\":2.3000,\"publicationDate\":\"2025-01-22\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Physics: Condensed Matter\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1088/1361-648X/ada47a\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"PHYSICS, CONDENSED MATTER\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Physics: Condensed Matter","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1088/1361-648X/ada47a","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"PHYSICS, CONDENSED MATTER","Score":null,"Total":0}
引用次数: 0

摘要

我们报道了La和Ru掺杂(Sr1-x Lax)2Ir1-xRuxO4 (x= 0.05, 0.15)的结构、磁性和电学性能的详细实验研究。x射线衍射分析表明,两种样品均呈四边形结晶结构,具有空间基I41/ add,不含杂质。La和Ru取代导致晶格参数a增大,c减小。随着掺杂浓度的增加,Ir-O- ir键角增大,Ir-O键长减小。x射线光电子能谱(XPS)表明,Ir具有Ir3+ (5d6)和Ir4+ (5d5)电荷态,其中Ir4+电荷态随着掺杂浓度的增加而降低。x= 0.05的直流磁化率(T)揭示了在TC ~ 229 K下由顺磁性(PM)向弱铁磁性(wFM)转变,这是由倾斜的AFM自旋排列引起的。高掺杂时,磁有序温度TC保持不变,但磁矩明显降低。基于传统的临界慢速模型、十年频移和Vogel-Fulcher定律分析了交流磁化率数据的实虚分量,一致证明了在x= 0.05的最低掺杂下存在可重入自旋玻璃行为(RSG),即弱铁磁性和自旋玻璃相共存。另一方面,对于空穴和电子的高掺杂(x=0.15),在x= 0.05时,在相同的温度下,RSG相消失,只留下wFM相。这表明La和Ru的高掺杂不影响磁性有序,但消除了FM和AFM相之间的无序。电阻率测量分析表明,两种样品在整个温度范围内都表现出半导体/绝缘行为。x= 0.05样品的比纯样品Sr2IrO4[1]低,而x= 0.15的在低温下比x= 0.05样品大两个数量级。用二维Mott变范围跳变(VRH)模型描述了两种样品的传导机理。我们的研究结果表明,两个阳离子位点的共掺杂产生了有趣的、竞争的跳跃和磁性过程。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Intriguing magnetic and electronic behaviors in La and Ru doped Sr2IrO4.

We report a detailed experimental study of the structural, magnetic and electrical properties of La and Ru doped (Sr1-xLax)2Ir1-xRuxO4(x= 0.05, 0.15). X-ray diffraction analysis reveals that both samples crystallize in a tetragonal structure with a space groupI41/acdwithout impurities. Substitution with La and Ru leads to an increase in the lattice parameteraand a decrease inc. With increasing doping concentration, the Ir-O-Ir bond angle increases while the Ir-O bond length decreases. X-ray photoelectron spectroscopy (XPS) shows that Ir has Ir3+(5d6) and Ir4+(5d5) charge states, where the Ir4+charge state decreases with an increase in doping concentration. Thedcmagnetic susceptibilityχ(T) ofx= 0.05 reveals a transition from paramagnetic to weak ferromagnetic (wFM) atTC∼ 229 K, arising from the canted antiferromagnetic (AFM) spin arrangement. The magnetic ordering temperatureTCremains unaltered for higher doping, whereas the magnetic moment is significantly reduced. The analysis of real and imaginary components ofacsusceptibility data, based on conventional critical slow model, frequency shift per decade and Vogel-Fulcher law, unanimously evidences the existence of reentrant spin-glass behavior (RSG), i.e. the coexistence of weak ferromagnetism and spin glass phases for the lowest doping ofx= 0.05. On the other hand, for higher doping (x= 0.15) of hole and electron, the RSG phase vanishes, leaving only the wFM phase at the same temperature as observed inx= 0.05. This suggests the higher doping of La and Ru does not affect the magnetic order, but removes the disorder between FM and AFM phases. The electrical resistivity (ρ) measurement analysis reveals that both the samples show semiconducting/insulating behavior across the temperature range. Theρof thex= 0.05 sample is lower than that of pure sample Sr2IrO4(Bhattiet al 2015 J. Phys.:Condens. Matter27016005), whileρofx= 0.15 shows two orders of magnitude larger than thex= 0.05 sample at low temperatures. The conduction mechanism of both samples is described by the 2D Mott's variable-range hopping model. Our results demonstrate that co-doping of two cation sites generates intriguing, competing hopping and magnetic processes.

求助全文
通过发布文献求助,成功后即可免费获取论文全文。 去求助
来源期刊
Journal of Physics: Condensed Matter
Journal of Physics: Condensed Matter 物理-物理:凝聚态物理
CiteScore
5.30
自引率
7.40%
发文量
1288
审稿时长
2.1 months
期刊介绍: Journal of Physics: Condensed Matter covers the whole of condensed matter physics including soft condensed matter and nanostructures. Papers may report experimental, theoretical and simulation studies. Note that papers must contain fundamental condensed matter science: papers reporting methods of materials preparation or properties of materials without novel condensed matter content will not be accepted.
×
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