{"title":"mgcu2型Laves相BaIr2在Ba5Ir7Ge4中的超导性","authors":"Terunari Koshinuma , Hiroshi Fujihisa , Yoshito Gotoh , Izumi Hase , Kenji Kawashima , Shigeyuki Ishida , Hiroshi Eisaki , Hiraku Ogino , Taichiro Nishio , Akira Iyo","doi":"10.1016/j.intermet.2025.108748","DOIUrl":null,"url":null,"abstract":"<div><div>We successfully synthesized the new compound Ba<sub>5</sub>Ir<sub>7</sub>Ge<sub>4</sub> at ambient pressure by adding Ge to BaIr<sub>2</sub>, which is a high-pressure stable MgCu<sub>2</sub>-type Laves phase. Rietveld analysis revealed that Ba<sub>5</sub>Ir<sub>7</sub>Ge<sub>4</sub> crystallizes by replacing part of the Ir<sub>4</sub> tetrahedra in BaIr<sub>2</sub> with Ge<sub>4</sub>Ir tetrahedra, forming in a network of corner-sharing Ge<sub>4</sub>Ir and Ir<sub>3</sub>Ge tetrahedra. While BaIr<sub>2</sub> has a cubic structure, Ba<sub>5</sub>Ir<sub>7</sub>Ge<sub>4</sub> adopts a new prototype structure with a tetragonal space group <em>I</em>4<sub>1</sub>/<em>a</em> (no.88) (<em>a</em> = 12.9726(2) Å, <em>c</em> = 8.2703(2) Å). Our experiments demonstrated that Ba<sub>5</sub>Ir<sub>7</sub>Ge<sub>4</sub> is a type-II superconductor with a transition temperature (<em>T</em><sub>c</sub>) of 3.2 K, which is slightly higher than that of BaIr<sub>2</sub>. Electronic structure calculations show that the density of states (DOS) at the Fermi energy is primarily contributed by the <em>d</em> states in the Ir atoms forming the Ir<sub>3</sub>Ge tetrahedra. Despite having smaller DOS at the Fermi level, Ba<sub>5</sub>Ir<sub>7</sub>Ge<sub>4</sub> exhibits a slightly higher <em>T</em><sub>c</sub> than that of BaIr<sub>2</sub>, which can be attributed to its higher Debye temperature.</div></div>","PeriodicalId":331,"journal":{"name":"Intermetallics","volume":"181 ","pages":"Article 108748"},"PeriodicalIF":4.3000,"publicationDate":"2025-03-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Superconductivity in Ba5Ir7Ge4 derived from MgCu2-type Laves phase BaIr2\",\"authors\":\"Terunari Koshinuma , Hiroshi Fujihisa , Yoshito Gotoh , Izumi Hase , Kenji Kawashima , Shigeyuki Ishida , Hiroshi Eisaki , Hiraku Ogino , Taichiro Nishio , Akira Iyo\",\"doi\":\"10.1016/j.intermet.2025.108748\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>We successfully synthesized the new compound Ba<sub>5</sub>Ir<sub>7</sub>Ge<sub>4</sub> at ambient pressure by adding Ge to BaIr<sub>2</sub>, which is a high-pressure stable MgCu<sub>2</sub>-type Laves phase. Rietveld analysis revealed that Ba<sub>5</sub>Ir<sub>7</sub>Ge<sub>4</sub> crystallizes by replacing part of the Ir<sub>4</sub> tetrahedra in BaIr<sub>2</sub> with Ge<sub>4</sub>Ir tetrahedra, forming in a network of corner-sharing Ge<sub>4</sub>Ir and Ir<sub>3</sub>Ge tetrahedra. While BaIr<sub>2</sub> has a cubic structure, Ba<sub>5</sub>Ir<sub>7</sub>Ge<sub>4</sub> adopts a new prototype structure with a tetragonal space group <em>I</em>4<sub>1</sub>/<em>a</em> (no.88) (<em>a</em> = 12.9726(2) Å, <em>c</em> = 8.2703(2) Å). Our experiments demonstrated that Ba<sub>5</sub>Ir<sub>7</sub>Ge<sub>4</sub> is a type-II superconductor with a transition temperature (<em>T</em><sub>c</sub>) of 3.2 K, which is slightly higher than that of BaIr<sub>2</sub>. Electronic structure calculations show that the density of states (DOS) at the Fermi energy is primarily contributed by the <em>d</em> states in the Ir atoms forming the Ir<sub>3</sub>Ge tetrahedra. Despite having smaller DOS at the Fermi level, Ba<sub>5</sub>Ir<sub>7</sub>Ge<sub>4</sub> exhibits a slightly higher <em>T</em><sub>c</sub> than that of BaIr<sub>2</sub>, which can be attributed to its higher Debye temperature.</div></div>\",\"PeriodicalId\":331,\"journal\":{\"name\":\"Intermetallics\",\"volume\":\"181 \",\"pages\":\"Article 108748\"},\"PeriodicalIF\":4.3000,\"publicationDate\":\"2025-03-22\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Intermetallics\",\"FirstCategoryId\":\"88\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S096697952500113X\",\"RegionNum\":2,\"RegionCategory\":\"材料科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"CHEMISTRY, PHYSICAL\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Intermetallics","FirstCategoryId":"88","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S096697952500113X","RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"CHEMISTRY, PHYSICAL","Score":null,"Total":0}
引用次数: 0
摘要
在高压稳定的mgcu2型Laves相BaIr2中加入Ge,成功合成了Ba5Ir7Ge4新化合物。Rietveld分析表明,Ba5Ir7Ge4通过用Ge4Ir四面体取代BaIr2中的部分Ir4四面体而结晶,形成一个共享角的Ge4Ir和Ir3Ge四面体网络。BaIr2为立方结构,而Ba5Ir7Ge4采用了具有四边形空间群I41/a (no.88)的新型原型结构(a = 12.9726(2) Å, c = 8.2703(2) Å)。我们的实验表明,Ba5Ir7Ge4是一种ii型超导体,其转变温度(Tc)为3.2 K,略高于BaIr2。电子结构计算表明,在费米能量处的态密度(DOS)主要由形成Ir3Ge四面体的Ir原子中的d态贡献。尽管Ba5Ir7Ge4在费米能级上的DOS较小,但其Tc略高于BaIr2,这可归因于其更高的德拜温度。
Superconductivity in Ba5Ir7Ge4 derived from MgCu2-type Laves phase BaIr2
We successfully synthesized the new compound Ba5Ir7Ge4 at ambient pressure by adding Ge to BaIr2, which is a high-pressure stable MgCu2-type Laves phase. Rietveld analysis revealed that Ba5Ir7Ge4 crystallizes by replacing part of the Ir4 tetrahedra in BaIr2 with Ge4Ir tetrahedra, forming in a network of corner-sharing Ge4Ir and Ir3Ge tetrahedra. While BaIr2 has a cubic structure, Ba5Ir7Ge4 adopts a new prototype structure with a tetragonal space group I41/a (no.88) (a = 12.9726(2) Å, c = 8.2703(2) Å). Our experiments demonstrated that Ba5Ir7Ge4 is a type-II superconductor with a transition temperature (Tc) of 3.2 K, which is slightly higher than that of BaIr2. Electronic structure calculations show that the density of states (DOS) at the Fermi energy is primarily contributed by the d states in the Ir atoms forming the Ir3Ge tetrahedra. Despite having smaller DOS at the Fermi level, Ba5Ir7Ge4 exhibits a slightly higher Tc than that of BaIr2, which can be attributed to its higher Debye temperature.
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