{"title":"场致 EuTe2 中的绝缘体-金属转变","authors":"Tetsuya Takeuchi, Fuminori Honda, Dai Aoki, Yoshinori Haga, Takanori Kida, Yasuo Narumi, Masayuki Hagiwara, Koichi Kindo, Kosuke Karube, Hisatomo Harima, Yoshichika Ōnuki","doi":"10.7566/jpsj.93.044708","DOIUrl":null,"url":null,"abstract":"We studied in detail the electrical and magnetic properties of the Eu-divalent antiferromagnet EuTe<sub>2</sub> with a tetragonal crystal structure using single crystals grown by the Te self-flux method. The observed anisotropic magnetization curves in the antiferromagnetic state below <i>T</i><sub>N</sub> = 11.1 K can be understood in terms of the magnetization processes of the two-sublattice model of an antiferromagnet with uniaxial magnetic anisotropy. A characteristic feature of this compound is that it becomes an insulator with decreasing temperature at zero magnetic field, but changes to a metal with a relatively low number of carriers in magnetic fields. From the results of magnetization, magnetoresistance, and Hall resistivity measurements in magnetic fields up to <i>μ</i><sub>0</sub><i>H</i> = 40 T, the insulator–metal transition was found to occur when the magnetization reaches ∼2 <i>μ</i><sub>B</sub>/Eu for both <tex-math space=\"preserve\" version=\"MathJax\">\\(H\\parallel [110]\\)</tex-math> and [001] at measurement temperatures above 50 K. Energy band calculations revealed that only the up-spin band, which is mainly composed of Te-5<i>p</i> electrons, crosses the Fermi level in the ferromagnetic state, although the energy band possesses a band gap in the paramagnetic and antiferromagnetic states.","PeriodicalId":17304,"journal":{"name":"Journal of the Physical Society of Japan","volume":"39 1","pages":""},"PeriodicalIF":1.5000,"publicationDate":"2024-03-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Field-induced Insulator–Metal Transition in EuTe2\",\"authors\":\"Tetsuya Takeuchi, Fuminori Honda, Dai Aoki, Yoshinori Haga, Takanori Kida, Yasuo Narumi, Masayuki Hagiwara, Koichi Kindo, Kosuke Karube, Hisatomo Harima, Yoshichika Ōnuki\",\"doi\":\"10.7566/jpsj.93.044708\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We studied in detail the electrical and magnetic properties of the Eu-divalent antiferromagnet EuTe<sub>2</sub> with a tetragonal crystal structure using single crystals grown by the Te self-flux method. The observed anisotropic magnetization curves in the antiferromagnetic state below <i>T</i><sub>N</sub> = 11.1 K can be understood in terms of the magnetization processes of the two-sublattice model of an antiferromagnet with uniaxial magnetic anisotropy. A characteristic feature of this compound is that it becomes an insulator with decreasing temperature at zero magnetic field, but changes to a metal with a relatively low number of carriers in magnetic fields. From the results of magnetization, magnetoresistance, and Hall resistivity measurements in magnetic fields up to <i>μ</i><sub>0</sub><i>H</i> = 40 T, the insulator–metal transition was found to occur when the magnetization reaches ∼2 <i>μ</i><sub>B</sub>/Eu for both <tex-math space=\\\"preserve\\\" version=\\\"MathJax\\\">\\\\(H\\\\parallel [110]\\\\)</tex-math> and [001] at measurement temperatures above 50 K. Energy band calculations revealed that only the up-spin band, which is mainly composed of Te-5<i>p</i> electrons, crosses the Fermi level in the ferromagnetic state, although the energy band possesses a band gap in the paramagnetic and antiferromagnetic states.\",\"PeriodicalId\":17304,\"journal\":{\"name\":\"Journal of the Physical Society of Japan\",\"volume\":\"39 1\",\"pages\":\"\"},\"PeriodicalIF\":1.5000,\"publicationDate\":\"2024-03-27\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of the Physical Society of Japan\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.7566/jpsj.93.044708\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"PHYSICS, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of the Physical Society of Japan","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.7566/jpsj.93.044708","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
摘要
我们利用 Te 自流式方法生长的单晶体,详细研究了具有四方晶体结构的 Eu 二价反铁磁体 EuTe2 的电学和磁学特性。在 TN = 11.1 K 以下的反铁磁态中观察到的各向异性磁化曲线可以从具有单轴磁性各向异性的反铁磁体的双子晶格模型的磁化过程来理解。这种化合物的一个特点是,在零磁场下,随着温度的降低,它变成了绝缘体,但在磁场中又变成了载流子数量相对较少的金属。从磁场高达 μ0H = 40 T 时的磁化、磁阻和霍尔电阻率测量结果来看,在测量温度高于 50 K 时,当 \(H\parallel [110]\) 和 [001] 的磁化率达到 ∼2 μB/Eu 时,绝缘体-金属转变就发生了。能带计算显示,尽管在顺磁态和反铁磁态中能带具有带隙,但在铁磁态中只有主要由 Te-5p 电子组成的上自旋带穿过费米级。
We studied in detail the electrical and magnetic properties of the Eu-divalent antiferromagnet EuTe2 with a tetragonal crystal structure using single crystals grown by the Te self-flux method. The observed anisotropic magnetization curves in the antiferromagnetic state below TN = 11.1 K can be understood in terms of the magnetization processes of the two-sublattice model of an antiferromagnet with uniaxial magnetic anisotropy. A characteristic feature of this compound is that it becomes an insulator with decreasing temperature at zero magnetic field, but changes to a metal with a relatively low number of carriers in magnetic fields. From the results of magnetization, magnetoresistance, and Hall resistivity measurements in magnetic fields up to μ0H = 40 T, the insulator–metal transition was found to occur when the magnetization reaches ∼2 μB/Eu for both \(H\parallel [110]\) and [001] at measurement temperatures above 50 K. Energy band calculations revealed that only the up-spin band, which is mainly composed of Te-5p electrons, crosses the Fermi level in the ferromagnetic state, although the energy band possesses a band gap in the paramagnetic and antiferromagnetic states.
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