{"title":"通过固溶体 Eu2Al15(Pt1-xT x )6 (T = Pd, Ir, Au; x = 1/6) 改变 Eu2Al15Pt6 中的价相转变","authors":"Stefan Engel, Lars Schumacher, Oliver Janka","doi":"10.1515/znb-2023-0072","DOIUrl":null,"url":null,"abstract":"Abstract The solid solutions Eu2Al15(Pt1−xT x )6 with T = Pd, Ir, Au and x = 1/6 were prepared by arc-melting the stoichiometric mixture of the elements, and subsequent annealing. For x = 1/6, all three solid solutions adopt the same structure type as Eu2Al15Pt6 according to powder X-ray diffraction data. Since the platinide Eu2Al15Pt6 exhibits a (3 + 1)D modulated structure (approximant in space group P121/m1), only the averaged hexagonal unit cell (P63/mmc, Sc0.6Fe2Si4.9 type) was refined by the Rietveld method. Scanning electron microscopy in combination with energy-dispersive X-ray spectroscopy (SEM/EDX) showed that the degree of substitution is in line with the weighed amounts. For values of x > 1/6, no phase-pure samples could be obtained. The results of the magnetic susceptibility measurements indicate that the isoelectronic substitution of Pd for Pt lowers the temperature of the first-order valence phase transition from Ttrans = 45 K in Eu2Al15Pt6 to Ttrans = 42 K in Eu2Al15(Pt5/6Pd1/6)6. For Eu2Al15(Pt5/6Ir1/6)6 and Eu2Al15(Pt5/6Au1/6)6 a change in the electronic situation occurs since the Ir substituted compound exhibits one electron less compared to the pristine Pt compound, while Eu2Al15(Pt5/6Au1/6)6 has one additional electron. As a consequence, Eu2Al15(Pt5/6Ir1/6)6 shows a higher valence phase transition temperature of Ttrans = 52 K while for Eu2Al15(Pt5/6Au1/6)6 no such transition is obvious.","PeriodicalId":23831,"journal":{"name":"Zeitschrift für Naturforschung B","volume":"21 19","pages":"21 - 27"},"PeriodicalIF":0.0000,"publicationDate":"2024-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Modifying the valence phase transition in Eu2Al15Pt6 by the solid solutions Eu2Al15(Pt1−xT x )6 (T = Pd, Ir, Au; x = 1/6)\",\"authors\":\"Stefan Engel, Lars Schumacher, Oliver Janka\",\"doi\":\"10.1515/znb-2023-0072\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Abstract The solid solutions Eu2Al15(Pt1−xT x )6 with T = Pd, Ir, Au and x = 1/6 were prepared by arc-melting the stoichiometric mixture of the elements, and subsequent annealing. For x = 1/6, all three solid solutions adopt the same structure type as Eu2Al15Pt6 according to powder X-ray diffraction data. Since the platinide Eu2Al15Pt6 exhibits a (3 + 1)D modulated structure (approximant in space group P121/m1), only the averaged hexagonal unit cell (P63/mmc, Sc0.6Fe2Si4.9 type) was refined by the Rietveld method. Scanning electron microscopy in combination with energy-dispersive X-ray spectroscopy (SEM/EDX) showed that the degree of substitution is in line with the weighed amounts. For values of x > 1/6, no phase-pure samples could be obtained. The results of the magnetic susceptibility measurements indicate that the isoelectronic substitution of Pd for Pt lowers the temperature of the first-order valence phase transition from Ttrans = 45 K in Eu2Al15Pt6 to Ttrans = 42 K in Eu2Al15(Pt5/6Pd1/6)6. For Eu2Al15(Pt5/6Ir1/6)6 and Eu2Al15(Pt5/6Au1/6)6 a change in the electronic situation occurs since the Ir substituted compound exhibits one electron less compared to the pristine Pt compound, while Eu2Al15(Pt5/6Au1/6)6 has one additional electron. As a consequence, Eu2Al15(Pt5/6Ir1/6)6 shows a higher valence phase transition temperature of Ttrans = 52 K while for Eu2Al15(Pt5/6Au1/6)6 no such transition is obvious.\",\"PeriodicalId\":23831,\"journal\":{\"name\":\"Zeitschrift für Naturforschung B\",\"volume\":\"21 19\",\"pages\":\"21 - 27\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Zeitschrift für Naturforschung B\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1515/znb-2023-0072\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Zeitschrift für Naturforschung B","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1515/znb-2023-0072","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
摘要
摘要 通过电弧熔炼元素的化学计量混合物并随后进行退火,制备了 T = Pd、Ir、Au 和 x = 1/6 的 Eu2Al15(Pt1-xT x )6 固溶体。对于 x = 1/6,根据粉末 X 射线衍射数据,所有三种固溶体都采用与 Eu2Al15Pt6 相同的结构类型。由于铂化物 Eu2Al15Pt6 显示出 (3 + 1)D 调制结构(空间群 P121/m1 的近似值),因此只用里特维尔德法对其平均六边形单胞(P63/mmc,Sc0.6Fe2Si4.9 型)进行了细化。扫描电子显微镜结合能量色散 X 射线光谱法(SEM/EDX)显示,替代程度与称重量一致。当 x 值 > 1/6 时,无法获得相纯样品。磁感应强度测量结果表明,铂对钯的等电子取代降低了一阶价相转变温度,从 Eu2Al15Pt6 中的 Ttrans = 45 K 降至 Eu2Al15(Pt5/6Pd1/6)6 中的 Ttrans = 42 K。Eu2Al15(Pt5/6Ir1/6)6和Eu2Al15(Pt5/6Au1/6)6的电子情况发生了变化,因为与原始铂化合物相比,Ir取代的化合物少了一个电子,而Eu2Al15(Pt5/6Au1/6)6则多了一个电子。因此,Eu2Al15(Pt5/6Ir1/6)6 的价相转变温度较高,为 Ttrans = 52 K,而 Eu2Al15(Pt5/6Au1/6)6 则没有明显的价相转变。
Modifying the valence phase transition in Eu2Al15Pt6 by the solid solutions Eu2Al15(Pt1−xT x )6 (T = Pd, Ir, Au; x = 1/6)
Abstract The solid solutions Eu2Al15(Pt1−xT x )6 with T = Pd, Ir, Au and x = 1/6 were prepared by arc-melting the stoichiometric mixture of the elements, and subsequent annealing. For x = 1/6, all three solid solutions adopt the same structure type as Eu2Al15Pt6 according to powder X-ray diffraction data. Since the platinide Eu2Al15Pt6 exhibits a (3 + 1)D modulated structure (approximant in space group P121/m1), only the averaged hexagonal unit cell (P63/mmc, Sc0.6Fe2Si4.9 type) was refined by the Rietveld method. Scanning electron microscopy in combination with energy-dispersive X-ray spectroscopy (SEM/EDX) showed that the degree of substitution is in line with the weighed amounts. For values of x > 1/6, no phase-pure samples could be obtained. The results of the magnetic susceptibility measurements indicate that the isoelectronic substitution of Pd for Pt lowers the temperature of the first-order valence phase transition from Ttrans = 45 K in Eu2Al15Pt6 to Ttrans = 42 K in Eu2Al15(Pt5/6Pd1/6)6. For Eu2Al15(Pt5/6Ir1/6)6 and Eu2Al15(Pt5/6Au1/6)6 a change in the electronic situation occurs since the Ir substituted compound exhibits one electron less compared to the pristine Pt compound, while Eu2Al15(Pt5/6Au1/6)6 has one additional electron. As a consequence, Eu2Al15(Pt5/6Ir1/6)6 shows a higher valence phase transition temperature of Ttrans = 52 K while for Eu2Al15(Pt5/6Au1/6)6 no such transition is obvious.