{"title":"Yb3+-畸变四边形Pr0.45Sr0.55MnO3的不可逆变磁跃迁","authors":"Ravi Kiran Dokala, Shaona Das, Ganesh Jangam, Pankaj Kumar Mishra, Subhash Thota","doi":"10.1088/1361-6463/ad030d","DOIUrl":null,"url":null,"abstract":"Abstract Field-induced metamagnetic behavior and orbital-ordering (OO) in Yb-substituted (PrSr)MnO 3 perovskites have been reported. The occurrence of distortions in the tetragonal crystal lattice leads to a reduction in the <?CDATA ${\\text{Mn}} - {{\\text{O}}_{\\left( 2 \\right)}} - {\\text{Mn}}$?> <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"> <mml:mrow> <mml:mtext>Mn</mml:mtext> </mml:mrow> <mml:mo>−</mml:mo> <mml:mrow> <mml:msub> <mml:mrow> <mml:mtext>O</mml:mtext> </mml:mrow> <mml:mrow> <mml:mfenced close=\")\" open=\"(\"> <mml:mn>2</mml:mn> </mml:mfenced> </mml:mrow> </mml:msub> </mml:mrow> <mml:mo>−</mml:mo> <mml:mrow> <mml:mtext>Mn</mml:mtext> </mml:mrow> </mml:math> bond angle, which in turn governs the temperature and field-dependent long-range magnetic orderings. Extensive magnetization measurements reveal the high Curie temperature <?CDATA ${T_{\\text{C}}}$?> <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"> <mml:mrow> <mml:msub> <mml:mi>T</mml:mi> <mml:mrow> <mml:mtext>C</mml:mtext> </mml:mrow> </mml:msub> </mml:mrow> </mml:math> ∼ 302 K ferromagnetic (FM) phase and suggest the possibility of the existence of the OO in Pr 0.45– x Yb x Sr 0.55 MnO 3 accompanied by antiferromagnetic (AFM) Néel temperature, <?CDATA ${T_{\\text{N}}}$?> <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"> <mml:mrow> <mml:msub> <mml:mi>T</mml:mi> <mml:mrow> <mml:mtext>N</mml:mtext> </mml:mrow> </mml:msub> </mml:mrow> </mml:math> , as low as 158 K. Irreversible metamagnetic transitions from the AFM phase to the FM phase occur for a specific composition x = 0.05 (Yb5) until <?CDATA $T$?> <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" overflow=\"scroll\"> <mml:mi>T</mml:mi> </mml:math> ⩽ 220 K. The admixture of AFM and FM metastable states is quite robust in the investigated system, whereas the AFM state is mediated by Yb 3+ ions, while the FM state arises as a result of field-driven thermo-magnetic kinetics. These results provide a constructive approach for designing novel spin-valve devices.","PeriodicalId":16833,"journal":{"name":"Journal of Physics D","volume":"13 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2023-10-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Irreversible Metamagnetic Transitions in Yb3+- distorted tetragonal Pr<sub>0.45</sub>Sr<sub>0.55</sub>MnO<sub>3</sub>\",\"authors\":\"Ravi Kiran Dokala, Shaona Das, Ganesh Jangam, Pankaj Kumar Mishra, Subhash Thota\",\"doi\":\"10.1088/1361-6463/ad030d\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Abstract Field-induced metamagnetic behavior and orbital-ordering (OO) in Yb-substituted (PrSr)MnO 3 perovskites have been reported. The occurrence of distortions in the tetragonal crystal lattice leads to a reduction in the <?CDATA ${\\\\text{Mn}} - {{\\\\text{O}}_{\\\\left( 2 \\\\right)}} - {\\\\text{Mn}}$?> <mml:math xmlns:mml=\\\"http://www.w3.org/1998/Math/MathML\\\" overflow=\\\"scroll\\\"> <mml:mrow> <mml:mtext>Mn</mml:mtext> </mml:mrow> <mml:mo>−</mml:mo> <mml:mrow> <mml:msub> <mml:mrow> <mml:mtext>O</mml:mtext> </mml:mrow> <mml:mrow> <mml:mfenced close=\\\")\\\" open=\\\"(\\\"> <mml:mn>2</mml:mn> </mml:mfenced> </mml:mrow> </mml:msub> </mml:mrow> <mml:mo>−</mml:mo> <mml:mrow> <mml:mtext>Mn</mml:mtext> </mml:mrow> </mml:math> bond angle, which in turn governs the temperature and field-dependent long-range magnetic orderings. Extensive magnetization measurements reveal the high Curie temperature <?CDATA ${T_{\\\\text{C}}}$?> <mml:math xmlns:mml=\\\"http://www.w3.org/1998/Math/MathML\\\" overflow=\\\"scroll\\\"> <mml:mrow> <mml:msub> <mml:mi>T</mml:mi> <mml:mrow> <mml:mtext>C</mml:mtext> </mml:mrow> </mml:msub> </mml:mrow> </mml:math> ∼ 302 K ferromagnetic (FM) phase and suggest the possibility of the existence of the OO in Pr 0.45– x Yb x Sr 0.55 MnO 3 accompanied by antiferromagnetic (AFM) Néel temperature, <?CDATA ${T_{\\\\text{N}}}$?> <mml:math xmlns:mml=\\\"http://www.w3.org/1998/Math/MathML\\\" overflow=\\\"scroll\\\"> <mml:mrow> <mml:msub> <mml:mi>T</mml:mi> <mml:mrow> <mml:mtext>N</mml:mtext> </mml:mrow> </mml:msub> </mml:mrow> </mml:math> , as low as 158 K. Irreversible metamagnetic transitions from the AFM phase to the FM phase occur for a specific composition x = 0.05 (Yb5) until <?CDATA $T$?> <mml:math xmlns:mml=\\\"http://www.w3.org/1998/Math/MathML\\\" overflow=\\\"scroll\\\"> <mml:mi>T</mml:mi> </mml:math> ⩽ 220 K. The admixture of AFM and FM metastable states is quite robust in the investigated system, whereas the AFM state is mediated by Yb 3+ ions, while the FM state arises as a result of field-driven thermo-magnetic kinetics. These results provide a constructive approach for designing novel spin-valve devices.\",\"PeriodicalId\":16833,\"journal\":{\"name\":\"Journal of Physics D\",\"volume\":\"13 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2023-10-30\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Physics D\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1088/1361-6463/ad030d\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Physics D","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1088/1361-6463/ad030d","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
摘要
本文报道了yb取代mno3钙钛矿的场致变磁性和轨道有序。四方晶格中畸变的发生导致Mn−o2−Mn键角的减小,这反过来又控制了温度和场相关的远程磁有序。广泛的磁化测量揭示了高居里温度T C ~ 302 K铁磁(FM)相,并表明在Pr 0.45 - x Yb x Sr 0.55 mno3中存在OO的可能性,并伴有低至158 K的反铁磁(AFM) n温度T N。对于特定成分x = 0.05 (Yb5),在T≤220 K之前,从AFM相到FM相发生不可逆的变磁转变。在所研究的体系中,AFM和FM亚稳态的混合非常稳定,而AFM状态是由yb3 +离子介导的,而FM状态是由场驱动的热磁动力学引起的。这些结果为设计新型自旋阀装置提供了建设性的思路。
Irreversible Metamagnetic Transitions in Yb3+- distorted tetragonal Pr0.45Sr0.55MnO3
Abstract Field-induced metamagnetic behavior and orbital-ordering (OO) in Yb-substituted (PrSr)MnO 3 perovskites have been reported. The occurrence of distortions in the tetragonal crystal lattice leads to a reduction in the Mn−O2−Mn bond angle, which in turn governs the temperature and field-dependent long-range magnetic orderings. Extensive magnetization measurements reveal the high Curie temperature TC ∼ 302 K ferromagnetic (FM) phase and suggest the possibility of the existence of the OO in Pr 0.45– x Yb x Sr 0.55 MnO 3 accompanied by antiferromagnetic (AFM) Néel temperature, TN , as low as 158 K. Irreversible metamagnetic transitions from the AFM phase to the FM phase occur for a specific composition x = 0.05 (Yb5) until T ⩽ 220 K. The admixture of AFM and FM metastable states is quite robust in the investigated system, whereas the AFM state is mediated by Yb 3+ ions, while the FM state arises as a result of field-driven thermo-magnetic kinetics. These results provide a constructive approach for designing novel spin-valve devices.