I. Grekhov, Y. Grishina, Zh Kurenbaeva, E. Murashova
{"title":"Rare earth ruthenium gallides with the high content of gallium LaRu2Ga3, R2Ru5Ga9 (RSm, Gd–Er) and R5Ru8Ga12 (RHo, Er)","authors":"I. Grekhov, Y. Grishina, Zh Kurenbaeva, E. Murashova","doi":"10.1016/j.jssc.2025.125442","DOIUrl":null,"url":null,"abstract":"<div><div>Compounds of the compositions LaRu<sub>2</sub>Ga<sub>3</sub>, R<sub>2</sub>Ru<sub>5</sub>Ga<sub>9</sub>, and R<sub>5</sub>Ru<sub>8</sub>Ga<sub>12</sub> were obtained close to the composition of RRu<sub>2</sub>Ga<sub>3</sub> in the R–Ru–Ga systems (R<img>La, Pr, Nd, Sm, Gd, Tb, Dy, Ho, and Er). The compound LaRu<sub>2</sub>Ga<sub>3</sub> crystallizes in its own structural type, R<sub>2</sub>Ru<sub>5</sub>Ga<sub>9</sub> (R<img>Sm, Gd–Er) crystallizes in the structural type Sm<sub>2</sub>Ru<sub>5</sub>Ga<sub>9</sub>, and R<sub>5</sub>Ru<sub>8</sub>Ga<sub>12</sub> (R<img>Ho, Er) crystallizes in a structural type derived from Sc<sub>5</sub>Re<sub>8</sub>Si<sub>12</sub>. The crystal structure of LaRu<sub>2</sub>Ga<sub>3</sub> is determined on a single crystal: <em>a</em> = 12.0750(12) Å, <em>b</em> = 5.8276(6) Å, <em>c</em> = 6.2391(6) Å, <em>V</em> = 439.03(8) Å<sup>3</sup>, Z = 4, space group <em>Pnma</em>. No new phases were found in samples with R<img>Pr, Nd. The crystal structure of R<sub>2</sub>Ru<sub>5</sub>Ga<sub>9</sub> was determined on a single crystal of one of the representatives of the series – Dy<sub>2</sub>Ru<sub>5</sub>Ga<sub>9</sub>: <em>a</em> = 6.1356(11) Å, <em>c</em> = 13.429(3) Å, <em>V</em> = 505.5(2) Å<sup>3</sup>, Z = 2, space group <em>I</em>4<em>/mmm</em>. The Ho<sub>5</sub>Ru<sub>8</sub>Ga<sub>12</sub> single crystal was used to determine the crystal structure: <em>a</em> = 15.332(2) Å, <em>b</em> = 20.019(3) Å, <em>c</em> = 5.4725(8) Å, <em>V</em> = 1679.7(4) Å<sup>3</sup>, Z = 4, space group <em>Fmm</em>2. Melting occurs congruently for all investigated compounds. It was not possible to obtain single phase samples for the determination of magnetic and electrically conductive properties.</div></div>","PeriodicalId":378,"journal":{"name":"Journal of Solid State Chemistry","volume":"349 ","pages":"Article 125442"},"PeriodicalIF":3.2000,"publicationDate":"2025-05-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Solid State Chemistry","FirstCategoryId":"92","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0022459625002658","RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"CHEMISTRY, INORGANIC & NUCLEAR","Score":null,"Total":0}
引用次数: 0
Abstract
Compounds of the compositions LaRu2Ga3, R2Ru5Ga9, and R5Ru8Ga12 were obtained close to the composition of RRu2Ga3 in the R–Ru–Ga systems (RLa, Pr, Nd, Sm, Gd, Tb, Dy, Ho, and Er). The compound LaRu2Ga3 crystallizes in its own structural type, R2Ru5Ga9 (RSm, Gd–Er) crystallizes in the structural type Sm2Ru5Ga9, and R5Ru8Ga12 (RHo, Er) crystallizes in a structural type derived from Sc5Re8Si12. The crystal structure of LaRu2Ga3 is determined on a single crystal: a = 12.0750(12) Å, b = 5.8276(6) Å, c = 6.2391(6) Å, V = 439.03(8) Å3, Z = 4, space group Pnma. No new phases were found in samples with RPr, Nd. The crystal structure of R2Ru5Ga9 was determined on a single crystal of one of the representatives of the series – Dy2Ru5Ga9: a = 6.1356(11) Å, c = 13.429(3) Å, V = 505.5(2) Å3, Z = 2, space group I4/mmm. The Ho5Ru8Ga12 single crystal was used to determine the crystal structure: a = 15.332(2) Å, b = 20.019(3) Å, c = 5.4725(8) Å, V = 1679.7(4) Å3, Z = 4, space group Fmm2. Melting occurs congruently for all investigated compounds. It was not possible to obtain single phase samples for the determination of magnetic and electrically conductive properties.
在R-Ru-Ga体系(RLa、Pr、Nd、Sm、Gd、Tb、Dy、Ho和Er)中,得到了与RRu2Ga3、R2Ru5Ga9和R5Ru8Ga12组成相近的化合物。化合物LaRu2Ga3结晶为自身结构类型,R2Ru5Ga9 (RSm, Gd-Er)结晶为Sm2Ru5Ga9结构类型,R5Ru8Ga12 (RHo, Er)结晶为Sc5Re8Si12衍生的结构类型。LaRu2Ga3的晶体结构在单晶上确定:a = 12.0750(12) Å, b = 5.8276(6) Å, c = 6.2391(6) Å, V = 439.03(8) Å3, Z = 4,空间群Pnma。在含有RPr、Nd的样品中未发现新的相。R2Ru5Ga9的晶体结构是在该系列代表之一的Dy2Ru5Ga9的单晶上确定的:a = 6.1356(11) Å, c = 13.429(3) Å, V = 505.5(2) Å3, Z = 2,空间群I4/mmm。用Ho5Ru8Ga12单晶测定晶体结构:a = 15.332(2) Å, b = 20.019(3) Å, c = 5.4725(8) Å, V = 1679.7(4) Å3, Z = 4,空间群Fmm2。所有被研究的化合物都一致地发生熔化。不可能获得单相样品来测定磁性和导电性。
期刊介绍:
Covering major developments in the field of solid state chemistry and related areas such as ceramics and amorphous materials, the Journal of Solid State Chemistry features studies of chemical, structural, thermodynamic, electronic, magnetic, and optical properties and processes in solids.