School of Physical Science and Technology, Southwest Jiaotong University, Chengdu 610031, PR China.
Inorg Chem. 2011 Oct 3;50(19):9256-65. doi: 10.1021/ic200337w. Epub 2011 Sep 6.
The trinuclear derivative Fe(3)(C(8)H(8))(3) was synthesized in 2009 by Lavallo and Grubbs via the reaction of Fe(C(8)H(8))(2) with a bulky heterocyclic carbene. This fascinating structure is the first example of a derivative of the well-known Fe(3)(CO)(12) in which all 12 carbonyl groups have been replaced by hydrocarbon ligands. The density functional theory predicts a structure having a central Fe(3) equilateral triangle with ∼2.9 Å Fe-Fe single bonded edges bridged by η(5),η(3)-C(8)H(8) ligands. This structure is close to the experimental structure, determined by X-ray crystallography. The related hypoelectronic M(3)(C(8)H(8))(3) derivatives (M = Cr, V, Ti) are predicted to have central scalene M(3) triangles with edge lengths and Wiberg bond indices (WBIs) corresponding to one formal single M-M bond, one formal double M═M bond, and one formal triple M≡M bond. For Mn(3)(C(8)H(8))(3), both a doublet structure with one Mn═Mn double bond and two Mn-Mn single bonds in the Mn(3) triangle, and a quartet structure with two Mn═Mn double bonds and one Mn-Mn single bond are predicted. The hyperelectronic derivatives M(3)(C(8)H(8))(3) have weaker direct M-M interactions in their M(3) triangles, as indicated by both the M-M distances and the WBIs. Thus, Ni(3)(C(8)H(8))(3) has bis(trihapto) η(3),η(3)-C(8)H(8) ligands bridging the edges of a central approximately equilateral Ni(3) triangle with long Ni···Ni distances of ∼3.7 Å. The WBIs indicate very little direct Ni-Ni bonding in this Ni(3) triangle and thus a local nickel environment in the singlet Ni(3)(C(8)H(8))(3) similar to that observed for diallylnickel (η(3)-C(3)H(5))(2)Ni.
2009 年,Lavallo 和 Grubbs 通过反应 Fe(C_8H_8)_2 与大位阻的杂环卡宾合成了三核衍生物 Fe(3)(C_8H_8)_3。这个引人入胜的结构是众所周知的 Fe(3)(CO)_12 的衍生物的第一个例子,其中所有 12 个羰基都被烃配体取代。密度泛函理论预测具有中心 Fe(3)等边三角形的结构,其中 ∼2.9 Å 的 Fe-Fe 单键边缘由 η(5),η(3)-C_8H_8 配体桥接。该结构与通过 X 射线晶体学确定的实验结构接近。相关的缺电子 M(3)(C_8H_8)_3 衍生物(M = Cr,V,Ti)被预测为具有中心不等边三角形的 M(3)三角形,其边长和 Wiberg 键指数(WBIs)对应于一个形式的单 M-M 键、一个形式的双 M═M 键和一个形式的三 M≡M 键。对于 Mn(3)(C_8H_8)_3,预测出两种结构,一种是具有一个 Mn═Mn 双键和 Mn(3)三角形中两个 Mn-Mn 单键的双重态结构,另一种是具有两个 Mn═Mn 双键和一个 Mn-Mn 单键的四重态结构。由于缺电子衍生物 M(3)(C_8H_8)_3 中 M(3)三角形的直接 M-M 相互作用较弱,如 M-M 距离和 WBIs 所示。因此,Ni(3)(C_8H_8)_3 具有双(三齿)η(3),η(3)-C_8H_8 配体桥接中心近似等边 Ni(3)三角形的边缘,Ni···Ni 距离约为 3.7 Å。WBIs 表明,在这个 Ni(3)三角形中几乎没有直接的 Ni-Ni 键合,因此在单重态 Ni(3)(C_8H_8)_3 中存在局部镍环境,类似于二烯镍(η(3)-C_3H_5)(2)Ni 中观察到的环境。