{"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}
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Abstract
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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