Feng Du, Lin Yang, Z. Nie, Ning Wu, Yong Li, S. Luo, Ye Chen, Dajun Su, Michael Smidman, Youguo Shi, C. Cao, Frank Steglich, Yunmei Song, H. Yuan
{"title":"E","authors":"Feng Du, Lin Yang, Z. Nie, Ning Wu, Yong Li, S. Luo, Ye Chen, Dajun Su, Michael Smidman, Youguo Shi, C. Cao, Frank Steglich, Yunmei Song, H. Yuan","doi":"10.1515/9783110580389-030","DOIUrl":null,"url":null,"abstract":"The combination of magnetic symmetries and electronic band topology provides a promising route for realizing topologically nontrivial quasiparticles, and the manipulation of magnetic structures may enable the switching between topological phases, with the potential for achieving functional physical properties. Here, we report measurements of the electrical resistivity of EuCd 2 As 2 under pressure, which show an intriguing insulating dome at pressures between p c1 ∼ 1 . 0 GPa and p c2 ∼ 2 . 0 GPa, situated between two regimes with metallic transport. The insulating state can be fully suppressed by a small magnetic field, leading to a colossal negative magnetoresistance on the order of 10 5 %, accessible via a modest field of ∼ 0 . 2 T. First-principles calculations reveal that the dramatic evolution of the resistivity under pressure is due to consecutive transitions of EuCd 2 As 2 from a magnetic topological insulator to a trivial insulator, and then to a Weyl semimetal, with the latter resulting from a pressure-induced change in the magnetic ground state. Similarly, the colossal magnetoresistance results from a field-induced polarization of the magnetic moments, transforming EuCd 2 As 2 from a trivial insulator to a Weyl semimetal. These findings underscore weak magnetic exchange couplings and spin anisotropy as ingredients for discovering tunable magnetic topological materials with desirable functionalities.","PeriodicalId":288401,"journal":{"name":"International Directory of Arts 2019","volume":"77 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2018-10-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"International Directory of Arts 2019","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1515/9783110580389-030","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
The combination of magnetic symmetries and electronic band topology provides a promising route for realizing topologically nontrivial quasiparticles, and the manipulation of magnetic structures may enable the switching between topological phases, with the potential for achieving functional physical properties. Here, we report measurements of the electrical resistivity of EuCd 2 As 2 under pressure, which show an intriguing insulating dome at pressures between p c1 ∼ 1 . 0 GPa and p c2 ∼ 2 . 0 GPa, situated between two regimes with metallic transport. The insulating state can be fully suppressed by a small magnetic field, leading to a colossal negative magnetoresistance on the order of 10 5 %, accessible via a modest field of ∼ 0 . 2 T. First-principles calculations reveal that the dramatic evolution of the resistivity under pressure is due to consecutive transitions of EuCd 2 As 2 from a magnetic topological insulator to a trivial insulator, and then to a Weyl semimetal, with the latter resulting from a pressure-induced change in the magnetic ground state. Similarly, the colossal magnetoresistance results from a field-induced polarization of the magnetic moments, transforming EuCd 2 As 2 from a trivial insulator to a Weyl semimetal. These findings underscore weak magnetic exchange couplings and spin anisotropy as ingredients for discovering tunable magnetic topological materials with desirable functionalities.
磁对称性和电子带拓扑的结合为实现拓扑非平凡准粒子提供了一条有前途的途径,对磁结构的操纵可能使拓扑相之间的切换成为可能,具有实现功能物理性质的潜力。在这里,我们报告了eucd2 As 2在压力下的电阻率测量结果,结果显示在pc1 ~ 1之间的压力下存在一个有趣的绝缘圆顶。0 GPa和p c2 ~ 2。0 GPa,位于两个具有金属输运的区域之间。绝缘状态可以被一个小的磁场完全抑制,导致一个巨大的负磁电阻,约为10.5%,通过一个适度的磁场达到~ 0。第一原理计算表明,压力下电阻率的急剧变化是由于eucd2 As 2从磁性拓扑绝缘体连续转变为普通绝缘体,然后转变为Weyl半金属,后者是由压力引起的磁性基态变化引起的。同样,巨大的磁阻是由磁场引起的磁矩极化引起的,将eucd2 As 2从普通绝缘体转变为Weyl半金属。这些发现强调弱磁交换耦合和自旋各向异性是发现具有理想功能的可调谐磁性拓扑材料的成分。