{"title":"具有以铂三角形为中心的 Sm 蜂窝结构的共线反铁磁体 SmPt6Al3","authors":"Ryohei Oishi, Yasuyuki Shimura, Kazunori Umeo, Takahiro Onimaru, Takeshi Matsumura, Mitsuru Tsukagoshi, Kenshin Kurauchi, Hiroto Nitta, Toshiro Takabatake","doi":"10.7566/jpsj.93.034707","DOIUrl":null,"url":null,"abstract":"We report a single-crystal study on the magnetism of the Sm honeycomb compound SmPt<sub>6</sub>Al<sub>3</sub> with the trigonal NdPt<sub>6</sub>Al<sub>3</sub>-type structure by the measurements of the magnetic susceptibility <i>χ</i>, electrical resistivity, specific heat, and resonant X-ray diffraction. The trivalent state of the Sm ion is indicated by the fact that the lattice parameters fall on the lanthanoid contraction lines for the <i>R</i><sup>3+</sup>Pt<sub>6</sub>Al<sub>3</sub> series. For <tex-math space=\"preserve\" version=\"MathJax\">\\(B\\parallel c\\)</tex-math>, <i>χ</i>(<i>T</i>) shows a cusp at <i>T</i><sub>N</sub> = 6.5 K and strongly decreases on cooling below <i>T</i><sub>N</sub>, whereas <i>χ</i>(<i>T</i>) for <tex-math space=\"preserve\" version=\"MathJax\">\\(B \\perp c\\)</tex-math> continues to increase without showing any anomaly at <i>T</i><sub>N</sub>. Application of <tex-math space=\"preserve\" version=\"MathJax\">\\(B\\parallel c\\)</tex-math> = 12 T depresses <i>T</i><sub>N</sub> to 4.6 K, whereas <i>T</i><sub>N</sub> remains at 6.4 K in <tex-math space=\"preserve\" version=\"MathJax\">\\(B \\perp c\\)</tex-math> = 14 T. The isothermal magnetization curves at 1.8 K for both <tex-math space=\"preserve\" version=\"MathJax\">\\(B\\parallel c\\)</tex-math> and <tex-math space=\"preserve\" version=\"MathJax\">\\(B \\perp c\\)</tex-math> have no spontaneous moment. These magnetic properties of SmPt<sub>6</sub>Al<sub>3</sub> indicate a collinear antiferromagnetic structure of the ordered moments pointing toward the <i>c</i> axis. This magnetic structure is verified by the Sm resonant X-ray diffraction measurement which revealed the <tex-math space=\"preserve\" version=\"MathJax\">\\([0,0,0]\\)</tex-math> propagation vector. By comparing the magnetic properties of SmPt<sub>6</sub>Al<sub>3</sub> with those for the canted antiferromagnet GdPt<sub>6</sub>Al<sub>3</sub>, we highlight the role of Dzyaloshinskii–Moriya interaction in the series of isostructural compounds with the centrosymmetric NdPt<sub>6</sub>Al<sub>3</sub>-type structure.","PeriodicalId":17304,"journal":{"name":"Journal of the Physical Society of Japan","volume":"16 1","pages":""},"PeriodicalIF":1.5000,"publicationDate":"2024-02-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Collinear Antiferromagnet SmPt6Al3 with a Sm Honeycomb Structure Centered by Pt Triangles\",\"authors\":\"Ryohei Oishi, Yasuyuki Shimura, Kazunori Umeo, Takahiro Onimaru, Takeshi Matsumura, Mitsuru Tsukagoshi, Kenshin Kurauchi, Hiroto Nitta, Toshiro Takabatake\",\"doi\":\"10.7566/jpsj.93.034707\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We report a single-crystal study on the magnetism of the Sm honeycomb compound SmPt<sub>6</sub>Al<sub>3</sub> with the trigonal NdPt<sub>6</sub>Al<sub>3</sub>-type structure by the measurements of the magnetic susceptibility <i>χ</i>, electrical resistivity, specific heat, and resonant X-ray diffraction. The trivalent state of the Sm ion is indicated by the fact that the lattice parameters fall on the lanthanoid contraction lines for the <i>R</i><sup>3+</sup>Pt<sub>6</sub>Al<sub>3</sub> series. For <tex-math space=\\\"preserve\\\" version=\\\"MathJax\\\">\\\\(B\\\\parallel c\\\\)</tex-math>, <i>χ</i>(<i>T</i>) shows a cusp at <i>T</i><sub>N</sub> = 6.5 K and strongly decreases on cooling below <i>T</i><sub>N</sub>, whereas <i>χ</i>(<i>T</i>) for <tex-math space=\\\"preserve\\\" version=\\\"MathJax\\\">\\\\(B \\\\perp c\\\\)</tex-math> continues to increase without showing any anomaly at <i>T</i><sub>N</sub>. Application of <tex-math space=\\\"preserve\\\" version=\\\"MathJax\\\">\\\\(B\\\\parallel c\\\\)</tex-math> = 12 T depresses <i>T</i><sub>N</sub> to 4.6 K, whereas <i>T</i><sub>N</sub> remains at 6.4 K in <tex-math space=\\\"preserve\\\" version=\\\"MathJax\\\">\\\\(B \\\\perp c\\\\)</tex-math> = 14 T. The isothermal magnetization curves at 1.8 K for both <tex-math space=\\\"preserve\\\" version=\\\"MathJax\\\">\\\\(B\\\\parallel c\\\\)</tex-math> and <tex-math space=\\\"preserve\\\" version=\\\"MathJax\\\">\\\\(B \\\\perp c\\\\)</tex-math> have no spontaneous moment. These magnetic properties of SmPt<sub>6</sub>Al<sub>3</sub> indicate a collinear antiferromagnetic structure of the ordered moments pointing toward the <i>c</i> axis. This magnetic structure is verified by the Sm resonant X-ray diffraction measurement which revealed the <tex-math space=\\\"preserve\\\" version=\\\"MathJax\\\">\\\\([0,0,0]\\\\)</tex-math> propagation vector. By comparing the magnetic properties of SmPt<sub>6</sub>Al<sub>3</sub> with those for the canted antiferromagnet GdPt<sub>6</sub>Al<sub>3</sub>, we highlight the role of Dzyaloshinskii–Moriya interaction in the series of isostructural compounds with the centrosymmetric NdPt<sub>6</sub>Al<sub>3</sub>-type structure.\",\"PeriodicalId\":17304,\"journal\":{\"name\":\"Journal of the Physical Society of Japan\",\"volume\":\"16 1\",\"pages\":\"\"},\"PeriodicalIF\":1.5000,\"publicationDate\":\"2024-02-26\",\"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.93.034707\",\"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.93.034707","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
我们报告了通过测量磁感应强度χ、电阻率、比热和共振 X 射线衍射,对具有三棱 NdPt6Al3 型结构的 Sm 蜂窝化合物 SmPt6Al3 的磁性进行的单晶研究。晶格参数落在 R3+Pt6Al3 系列的镧系收缩线上这一事实表明了 Sm 离子的三价态。对于\(B\parallel c\), χ(T)在TN = 6.5 K时显示出一个尖点,并且在低于TN时随着冷却而强烈减小,而对于\(B\perp c\), χ(T)继续增大,在TN处没有显示出任何异常。应用 \(B\parallel c\) = 12 T 时,TN 下降到 4.6 K,而 \(B\perp c\) = 14 T 时,TN 保持在 6.4 K。SmPt6Al3 的这些磁性能表明,有序磁矩指向 c 轴的共线反铁磁结构。这种磁性结构通过 Sm 共振 X 射线衍射测量得到了验证,测量结果显示了 \([0,0,0]\) 传播矢量。通过将 SmPt6Al3 的磁性能与有尖角反铁磁体 GdPt6Al3 的磁性能进行比较,我们强调了 Dzyaloshinskii-Moriya 相互作用在具有中心对称 NdPt6Al3 型结构的等结构化合物系列中的作用。
Collinear Antiferromagnet SmPt6Al3 with a Sm Honeycomb Structure Centered by Pt Triangles
We report a single-crystal study on the magnetism of the Sm honeycomb compound SmPt6Al3 with the trigonal NdPt6Al3-type structure by the measurements of the magnetic susceptibility χ, electrical resistivity, specific heat, and resonant X-ray diffraction. The trivalent state of the Sm ion is indicated by the fact that the lattice parameters fall on the lanthanoid contraction lines for the R3+Pt6Al3 series. For \(B\parallel c\), χ(T) shows a cusp at TN = 6.5 K and strongly decreases on cooling below TN, whereas χ(T) for \(B \perp c\) continues to increase without showing any anomaly at TN. Application of \(B\parallel c\) = 12 T depresses TN to 4.6 K, whereas TN remains at 6.4 K in \(B \perp c\) = 14 T. The isothermal magnetization curves at 1.8 K for both \(B\parallel c\) and \(B \perp c\) have no spontaneous moment. These magnetic properties of SmPt6Al3 indicate a collinear antiferromagnetic structure of the ordered moments pointing toward the c axis. This magnetic structure is verified by the Sm resonant X-ray diffraction measurement which revealed the \([0,0,0]\) propagation vector. By comparing the magnetic properties of SmPt6Al3 with those for the canted antiferromagnet GdPt6Al3, we highlight the role of Dzyaloshinskii–Moriya interaction in the series of isostructural compounds with the centrosymmetric NdPt6Al3-type structure.
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