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Nine Hexagonal Ca5Pb3Z Phases in Stuffed Mn5Si3-Type Structures with Transition Metal Interstitial Atoms Z. Problems with Classical Valence States in Possible Zintl Phases

机译:具有过渡金属间隙原子Z的Mn5Si3型填充结构中的九个六角形Ca5Pb3Z相。可能的Zintl相具有经典价态的问题

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摘要

Ternary hexagonal Ae5Tt3Z phases have been obtained from high-temperature reactions (1000−1300 °C in Ta) only for Ae (alkaline-earth metal) = Ca, Tt (tetrel) = Pb, and Z = V, Cr, Mn, Fe, Co, Ni, Zn, Ru, or Cd. The hexagonal crystal structures (stuffed Mn5Si3-type, P63/mcm, Z = 2) were refined for Z = Mn and Fe (a = 9.3580(3), 9.3554(5) Å, c = 7.009(1), 7.009(1) Å, respectively). In contrast, Ca5Pb3Z for Z = Cu or Ag form only with a trigonal structure (P3̄c1, Z = 2, a = 9.4130(3) Å, c = 7.052(1) Å for Cu) in which regular displacements of only the linear strings of Ca1 atoms occur. The existence of these compounds stands in contrast to the nonexistence of all binary Ae5Tt3 products from Ca to Ba (Ae) and Si to Pb (Tt) with a Mn5Si3-type structure. Therefore, it once seemed attractive to consider the Z elements in these Ca5Pb3Z compounds as reducing agents (electron donors). The Mn and Fe structures appropriately exhibit greatly enlarged antiprismatic calcium cavities about Z. Other indications of relatively electron-poor environments around Fe are found in its properties, which include soft ferromagnetism with an elevated magnetic moment (6.3 μB) and a large Fe 3p3/2 binding energy relative to that in La5Ge3Fe, La15Ge9Fe, etc. The Ca5Pb3Mn phase exhibits metallic behavior (ρ295 = 135 μΩ cm) and temperature-independent Pauli paramagnetism. These properties are supported by ab initio band structure calculations for Ca5Pb3Mn, which show strong Ca−Pb bonding and a broad Pb-based band, with appreciable Ca−Mn and Ca−Pb bonding states at and above EF. Distortion of the Cu analogue gives strengthened Ca−Pb bonding and reduced Cu−Ca1 repulsions. A Zintl phase description of these compounds and some releated compounds in terms of closed Pb bands is not appropriate.
机译:仅对于Ae(碱土金属)= Ca,Tt(tetrel)= Pb和Z = V,Cr,Mn,Fe的高温反应(Ta-1000-1300°C,Ta中)获得三元六方Ae5Tt3Z相,Co,Ni,Zn,Ru或Cd。精制Z = Mn和Fe(a = 9.3580(3),9.3554(5)Å,c = 7.009(1),7.009(1)的六方晶体结构(填充Mn5Si3型,P63 / mcm,Z = 2) )Å)。相反,对于Z = Cu或Ag,Ca5Pb3Z仅具有三角结构(P3̄c1,Z = 2,对于Cu = a = 9.4130(3)Å,对于c = 7.052(1)Å),其中仅线性串的规则位移发生Ca1原子。这些化合物的存在与不存在具有Mn5Si3型结构的从Ca到Ba(Ae)和Si到Pb(Tt)的所有二元Ae5Tt3产物相反。因此,曾经将这些Ca5Pb3Z化合物中的Z元素视为还原剂(电子给体)似乎很有吸引力。 Mn和Fe结构适当地在Z周围表现出极大的反棱镜钙腔。在Fe周围的特性中还发现了相对电子贫乏的环境的其他迹象,包括具有较高磁矩(6.3μB)的软铁磁性和较大的Fe 3p3 /相对于La5Ge3Fe,La15Ge9Fe等,结合能为2。Ca5Pb3Mn相表现出金属行为(ρ295= 135μΩcm)和不依赖温度的Pauli顺磁性。这些性质得到了Ca5Pb3Mn的从头算带结构计算的支持,该计算显示出强的Ca-Pb键和宽的Pb基带,并且在EF或以上具有明显的Ca-Mn和Ca-Pb键态。铜类似物的变形会增强Ca-Pb的结合力,并减少Cu-Ca1的排斥力。这些化合物和某些相关化合物在封闭的Pb带上的Zintl相描述是不合适的。

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