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}
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.
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.