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Superconductivity in Y4RuGe8 with a Vacancy-Ordered CeNiSi2-Type Superstructure
Chemistry of Materials ( IF 8.6 ) Pub Date : 2021-09-24 , DOI: 10.1021/acs.chemmater.1c02488
Jin-Ke Bao 1, 2 , Huihuo Zheng 3 , Jianguo Wen 4 , Sitaram Ramakrishnan 2, 5 , Hao Zheng 6 , Jidong Samuel Jiang 1 , Daniel Bugaris 1 , Gang Cao 6 , Duck Young Chung 1 , Sander van Smaalen 2 , Mercouri G. Kanatzidis 1, 7
Affiliation  

We report a new compound, Y4RuGe8, with a transition metal vacancy-ordered CeNiSi2-type superstructure, which has a superconducting transition at 1.3 K. Y4RuGe8 crystals were grown by indium flux at relatively low temperatures (below 1273 K), which makes it possible to stabilize such a vacancy-ordered phase. The crystal structure of Y4RuGe8 was solved by single-crystal X-ray diffraction and confirmed by transmission electron microscopy. The as-grown Y4RuGe8 crystals are always twinned, crystallizing in the space group P1̅ (no. 2) with the lattice parameters a = 5.7680(1) Å, b = 8.2042(2) Å, c = 11.5093(3) Å, α = 79.696(1)°, β = 88.491(1)°, and γ = 79.637(2)°; this structure is a superstructure deriving from the higher symmetry CeNiSi2-type structure (Cmcm, no. 63) due to the ordering of Ru vacancies. The ordering of Ru sites breaks slightly distorted Ge planes in the CeNiSi2 prototype into infinite cis–trans Ge chains in Y4RuGe8. The presence of bulk superconductivity in Y4RuGe8 is well supported by zero resistance and a jump in specific heat at the critical transition temperature. The Sommerfeld coefficient (19 mJ K–2 mol–1) of the specific heat is greater than that (11 mJ K–2 mol–1) estimated using the bare density of states (4.7 states/eV/f.u.) from first-principles calculations. The ab initio calculations indicate that 4d electrons of both Y and Ru and 4p electrons of Ge are the main contributors to the total density of states at the Fermi level in Y4RuGe8.

中文翻译:

具有空位有序 CeNiSi2 型超结构的 Y4RuGe8 中的超导性

我们报告了一种新化合物 Y 4 RuGe 8,它具有过渡金属空位有序的 CeNiSi 2型超结构,在 1.3 K 下具有超导转变。 Y 4 RuGe 8晶体是在相对较低的温度下(低于 1273 K),这使得稳定这种空位有序相成为可能。Y 4 RuGe 8的晶体结构通过单晶X射线衍射解析并通过透射电子显微镜确认。生长的 Y 4 RuGe 8晶体总是孪晶,在空间群P 1̅ (no. 2) 中结晶,晶格参数为a= 5.7680(1) Å,b = 8.2042(2) Å,c = 11.5093(3) Å,α = 79.696(1)°,β = 88.491(1)°,γ = 79.637(2)°;由于 Ru 空位的排序,该结构是源自更高对称性的 CeNiSi 2型结构(Cmcm,第 63 号)的超结构。Ru位点的排序将CeNiSi 2原型中略微扭曲的Ge平面分解为Y 4 RuGe 8 中的无限顺-反Ge链。Y 4 RuGe 8中体超导性的存在得到零电阻和临界转变温度下比热跳跃的良好支持。索末菲系数 (19 mJ K –2 mol–1 ) 的比热大于使用第一性原理计算的裸态密度 (4.7 态/eV/fu) 估计的比热 (11 mJ K –2 mol –1 )。的从头计算表明,两个Y和Ru和4P电子Ge中的4D电子是主要贡献者状态中的Y中的费米能级的总密度4卢格8
更新日期:2021-10-12
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