Department of Chemistry, Iowa State University, Ames, Iowa 50011, USA.
Inorg Chem. 2013 Feb 4;52(3):1328-37. doi: 10.1021/ic301933a. Epub 2013 Jan 16.
The region of the Au-Zn phase diagram encompassing γ-brass-type phases has been studied experimentally from 45 to 85 atom % Zn. The γ phases were obtained directly from the pure elements by heating to 680 °C in evacuated silica tubes, followed by annealing at 300 °C. Powder X-ray and single-crystal diffraction studies show that γ-"Au(5)Zn(8)" phases adopt a rhombohedrally distorted Cr(5)Al(8) structure type rather than the cubic Cu(5)Zn(8) type. The refined compositions from two single crystals extracted from the Zn- and Au-rich loadings are Au(4.27(3))Zn(8.26(3))□(0.47) (I) and Au(4.58(3))Zn(8.12(3))□(0.3) (II), respectively (□ = vacancy). These (I and II) refinements indicated both nonstatistical mixing of Au and Zn atoms as well as partially ordered vacancy distributions. The structures of these γ phases were solved in the acentric space group R3m (No. 160, Z = 6), and the observed lattice parameters from powder patterns were found to be a = 13.1029(6) and 13.1345(8) Å and c = 8.0410(4) and 8.1103(6) Å for crystals I and II, respectively. According to single-crystal refinements, the vacancies were found on the outer tetrahedron (OT) and octahedron (OH) of the 26-atom cluster. Single-crystal structural refinement clearly showed that the vacancy content per unit cell increases with increasing Zn, or valence-electron concentration. Electronic structure calculations, using the tight-binding linear muffin-tin orbital method with the atomic-sphere approximation (TB-LMTO-ASA) method, indicated the presence of a well-pronounced pseudogap at the Fermi level for "Au(5)Zn(8)" as the representative composition, an outcome that is consistent with the Hume-Rothery interpretation of γ brass.
从 45 到 85 原子%的锌,对包括 γ-黄铜型相的 Au-Zn 相图区域进行了实验研究。γ 相是通过在真空中的硅管中加热至 680°C 直接从纯元素获得的,然后在 300°C 下退火。粉末 X 射线和单晶衍射研究表明,γ-"Au(5)Zn(8)" 相采用了具有菱面体畸变的 Cr(5)Al(8)结构类型,而不是立方 Cu(5)Zn(8)类型。从富锌和富金负载中提取的两个单晶的精细成分分别为 Au(4.27(3))Zn(8.26(3))□(0.47)(I)和 Au(4.58(3))Zn(8.12(3))□(0.3)(II)(□=空位)。这些(I 和 II)细化表明 Au 和 Zn 原子的非统计混合以及部分有序空位分布。这些 γ 相的结构在非中心空间群 R3m(No.160,Z=6)中得到了解决,从粉末图谱中观察到的晶格参数分别为 a=13.1029(6)和 13.1345(8)Å和 c=8.0410(4)和 8.1103(6)Å,对于晶体 I 和 II。根据单晶细化,空位位于 26 原子簇的外四面体(OT)和八面体(OH)上。单晶结构细化清楚地表明,空位含量随 Zn 或价电子浓度的增加而增加。使用原子球近似(TB-LMTO-ASA)方法的紧束缚线性 muffin-tin 轨道方法的电子结构计算表明,对于代表性组成“Au(5)Zn(8)”,费米能级处存在明显的赝隙,这与 Hume-Rothery 对 γ 黄铜的解释一致。