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gamma_l-Pt_5Zn_(21)--a reappraisal of a gamma-brass type complex alloy phase

机译:gamma_l-Pt_5Zn_(21)-对γ-黄铜型复合合金相的重新评估

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The constitution of the gamma-phase field in the Pt-Zn system was reinvestigated. The samples were prepared from the elements in sealed silica tubes at 1320 K followed by slow cooling to 970 K. Three structurally distinct gamma-phases were identified by means of single crystal X-ray diffraction. The gamma_1- and gamma'_1-phase represent two structurally intimately related 2a X 2a X 2a superstructures of the ordinary gamma -Pt_2Zn_(10.75). Three crystal structures were refined from single crystal intensity data: gamma_1-Pt_(5.12)Zn_(20.47)(F4-(bar)3m, a = 1809.1(1) pm, cF416-6.6, R_F = 0.043), gamma_1-Pt_(4.72)Zn_(20.92) (F4-(bar)3m, a = 1812.8(2) pm, cF416-5.8, R_F = 0.034), and gamma'_-Pt_(4.25)Zn_(20.34) (F4-(bar)3m, a = 1814.0(1) pm, cF416-22.7, R_F = 0.054). The structures are discussed in terms of four symmetrically inequivalent 26 atom clusters each comprising inner tetrahedral (IT), outer tetrahedral (OT), octahedral (OH) and cuboctahedral (CO) positions. The homogeneity range of the gamma_1-phase extends between 18.4 and 20.0 at. percent Pt, a range which encompasses the composition Pt_5Zn_(21). Two symmetrically independent, ordered Pt_4Zn_(22) clusters form the compositionally invariant part of the structure. Two complementary, partly disordered Pt_(6+-delta)Zn_(20-delta), clusters account for the homogeneity range of the phase. They vary in composition due to mutual Pt/Zn substitution, vacancies at Zn sites, and partial positional disorder. The closely related phase gamma'_1-Pt_(4.25)Zn_(20.34) is separated from the gamma_-phase by a small miscibility gap which is indicated by isopiestic measurements and a discontinuous jump of the vacancy concentration. The melting point of the phases increases with rise of the Pt content: 1136(2) K (gamma), 1238(5) K(gamma'_1) and 1251(3) K (gamma_1). The magnetic susceptibility is dominated by the core diamagnetism of the constituents. chi_(mol) was found to vary between -4.7 X 10~(-10) and -3.1 X 10~(-10) m~3 mol~(-1).
机译:再次研究了Pt-Zn体系中γ相场的构成。由密封的石英管中的元素在1320 K下制备样品,然后缓慢冷却至970K。通过单晶X射线衍射鉴定出三个结构不同的γ相。 γ_1-相和γ'_1-相表示普通γ-Pt_2Zn_(10.75)的两个结构紧密相关的2a X 2a X 2a超结构。从单晶强度数据中提炼出三种晶体结构:gamma_1-Pt_(5.12)Zn_(20.47)(F4-(bar)3m,a = 1809.1(1)pm,cF416-6.6,R_F = 0.043),gamma_1-Pt_( 4.72)Zn_(20.92)(F4-(bar)3m,a = 1812.8(2)pm,cF416-5.8,R_F = 0.034)和gamma'_- Pt_(4.25)Zn_(20.34)(F4-(bar) 3m,a = 1814.0(1)pm,cF416-22.7,R_F = 0.054)。根据四个对称不等价的26个原子簇讨论了结构,每个簇包含内部四面体(IT),外部四面体(OT),八面体(OH)和立方八面体(CO)位置。 γ_1相的均匀范围在18.4和20.0 at之间。 Pt百分比,包含组成Pt_5Zn_(21)的范围。两个对称独立的,有序的Pt_4Zn_(22)簇形成了结构的组成不变部分。两个互补的,部分无序的Pt_(6 +-δ)Zn_(20-δ)簇说明了相的均匀性范围。由于相互之间的Pt / Zn取代,Zn位点的空位以及部分位置的混乱,它们的成分有所不同。紧密相关的相γ'_1-Pt_(4.25)Zn_(20.34)通过小的溶混间隙与γ相分离,这由同晶测量和空位浓度的不连续跃变指示。相的熔点随Pt含量的增加而增加:1136(2)K(γ),1238(5)K(γ′_1)和1251(3)K(γ_1)。磁化率主要由成分的磁抗磁性决定。发现chi_(mol)在-4.7 X 10〜(-10)和-3.1 X 10〜(-10)m〜3 mol〜(-1)之间变化。

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