{"title":"基于 3d-5db 的双包晶石 Nd2-xSrxCoIrO6 的结构、磁性和传输特性的演变。","authors":"Raktim Datta, Suman Mondal, Suchanda Mondal, Suman Kalyan Pradhan, Subham Majumdar, Subodh Kumar De","doi":"10.1088/1361-648X/ad8d9b","DOIUrl":null,"url":null,"abstract":"<p><p>The evolution of the structural, magnetic and transport properties of the intermediate compounds Nd2-xSr<sub><i>x</i></sub>CoIrO<sub>6</sub>with<i>x</i>= 0.2, 0.4, 0.6, 1 and 1.5 have been studied to establish important roles of sizes and oxidation states of cations on various phases. The replacement of Nd<sup>3+</sup>by Sr<sup>2+</sup>primarily influences the oxidation states of Co (Co<sup>2+</sup>→Co<sup>3+</sup>) and Ir (Ir<sup>4+</sup>→Ir<sup>5+</sup>) ions to maintain the charge neutrality in the entire system. The Sr dopants give rise to an increasing Co/Ir antisite disorder (ASD) to accommodate the variation of charge state and ionic radius of Co and Ir. The nature of magnetic interaction induced by Sr changes from being a ferrimagnetic (FIM) to a more dominant antiferromagnetic. The suppression of the second magnetic transition below 30 K in samples for<i>x</i>>0.2 is entirely due to dilution of the Nd-Nd magnetic interaction. The combined effects of ASD and mixed oxidation state of Co and Ir ions generate various types of magnetic exchange pathways and create competitive magnetic interactions to stabilize a particular magnetic ground state. In the middle compound NdSrCoIrO<sub>6</sub>, a Griffith like phase in the temperature region 65-150 K and exchange bias field of 658 Oe at 2.3 K under a cooling field of 50 kOe has been observed. The compounds show an insulating kind of behaviour, and with hole doping the value of room temperature resistivity drastically decreases. The nature of conduction is found to follow three dimensional Mott's variable range hopping process.</p>","PeriodicalId":16776,"journal":{"name":"Journal of Physics: Condensed Matter","volume":"37 6","pages":""},"PeriodicalIF":2.3000,"publicationDate":"2024-11-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Evolution of structural, magnetic and transport properties of 3<i>d</i>-5<i>d</i>based double perovskites Nd<sub>2-<i>x</i></sub>Sr<sub><i>x</i></sub>CoIrO<sub>6</sub>.\",\"authors\":\"Raktim Datta, Suman Mondal, Suchanda Mondal, Suman Kalyan Pradhan, Subham Majumdar, Subodh Kumar De\",\"doi\":\"10.1088/1361-648X/ad8d9b\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p><p>The evolution of the structural, magnetic and transport properties of the intermediate compounds Nd2-xSr<sub><i>x</i></sub>CoIrO<sub>6</sub>with<i>x</i>= 0.2, 0.4, 0.6, 1 and 1.5 have been studied to establish important roles of sizes and oxidation states of cations on various phases. The replacement of Nd<sup>3+</sup>by Sr<sup>2+</sup>primarily influences the oxidation states of Co (Co<sup>2+</sup>→Co<sup>3+</sup>) and Ir (Ir<sup>4+</sup>→Ir<sup>5+</sup>) ions to maintain the charge neutrality in the entire system. The Sr dopants give rise to an increasing Co/Ir antisite disorder (ASD) to accommodate the variation of charge state and ionic radius of Co and Ir. The nature of magnetic interaction induced by Sr changes from being a ferrimagnetic (FIM) to a more dominant antiferromagnetic. The suppression of the second magnetic transition below 30 K in samples for<i>x</i>>0.2 is entirely due to dilution of the Nd-Nd magnetic interaction. The combined effects of ASD and mixed oxidation state of Co and Ir ions generate various types of magnetic exchange pathways and create competitive magnetic interactions to stabilize a particular magnetic ground state. In the middle compound NdSrCoIrO<sub>6</sub>, a Griffith like phase in the temperature region 65-150 K and exchange bias field of 658 Oe at 2.3 K under a cooling field of 50 kOe has been observed. The compounds show an insulating kind of behaviour, and with hole doping the value of room temperature resistivity drastically decreases. 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引用次数: 0
摘要
研究了中间化合物 Nd2-xSrxCoIrO6(x= 0.2、0.4、0.6、1 和 1.5)的结构、磁性和传输特性的演变,以确定阳离子的大小和氧化态对各种相的重要作用。用 Sr2+ 替代 Nd3+ 主要影响 Co(Co2+→Co3+)和 Ir(Ir4+→Ir5+)离子的氧化态,以保持整个体系的电荷中性。掺杂锶会导致 Co/Ir 反斜面无序度 (ASD) 增加,以适应 Co 和 Ir 的电荷状态和离子半径的变化。Sr 诱导的磁性相互作用的性质从铁磁性(FIM)转变为更主要的反铁磁性。在 x>0.2 的样品中,30 K 以下第二磁转变的抑制完全是由于 Nd-Nd 磁相互作用的稀释。ASD 和 Co、Ir 离子混合氧化态的共同作用产生了各种类型的磁交换途径,并产生了竞争性的磁相互作用以稳定特定的磁基态。在中间化合物 NdSrCoIrO6 中,在 65-150 K 的温度区域和 658 Oe 的交换偏置磁场(2.3 K,冷却磁场为 50 kOe)下观察到了类似格里菲斯相的现象。这些化合物显示出一种绝缘行为,随着空穴掺杂,室温电阻率值急剧下降。发现传导性质遵循三维莫特变程跳变过程。
Evolution of structural, magnetic and transport properties of 3d-5dbased double perovskites Nd2-xSrxCoIrO6.
The evolution of the structural, magnetic and transport properties of the intermediate compounds Nd2-xSrxCoIrO6withx= 0.2, 0.4, 0.6, 1 and 1.5 have been studied to establish important roles of sizes and oxidation states of cations on various phases. The replacement of Nd3+by Sr2+primarily influences the oxidation states of Co (Co2+→Co3+) and Ir (Ir4+→Ir5+) ions to maintain the charge neutrality in the entire system. The Sr dopants give rise to an increasing Co/Ir antisite disorder (ASD) to accommodate the variation of charge state and ionic radius of Co and Ir. The nature of magnetic interaction induced by Sr changes from being a ferrimagnetic (FIM) to a more dominant antiferromagnetic. The suppression of the second magnetic transition below 30 K in samples forx>0.2 is entirely due to dilution of the Nd-Nd magnetic interaction. The combined effects of ASD and mixed oxidation state of Co and Ir ions generate various types of magnetic exchange pathways and create competitive magnetic interactions to stabilize a particular magnetic ground state. In the middle compound NdSrCoIrO6, a Griffith like phase in the temperature region 65-150 K and exchange bias field of 658 Oe at 2.3 K under a cooling field of 50 kOe has been observed. The compounds show an insulating kind of behaviour, and with hole doping the value of room temperature resistivity drastically decreases. The nature of conduction is found to follow three dimensional Mott's variable range hopping process.
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.