Lerayer Emmanuel, Renaut Patrice, Brandès Stéphane, Cattey Hélène, Fleurat-Lessard Paul, Bouhadir Ghenwa, Bourissou Didier, Hierso Jean-Cyrille
Université de Bourgogne Franche-Comté , Institut de Chimie Moléculaire de l'Université de Bourgogne (ICMUB UMR 6302 CNRS), 9 Avenue Alain Savary, 21078 Dijon, France.
Laboratoire Hétérochimie Fondamentale et Appliquée (LHFA), Université Paul Sabatier/CNRS UMR 5069 , 118 Route de Narbonne, 31062 Toulouse, Cedex 09, France.
Inorg Chem. 2017 Feb 20;56(4):1966-1973. doi: 10.1021/acs.inorgchem.6b02510. Epub 2017 Jan 31.
The reaction of nonsubstituted alkali metal cyclopentadienides with haloboranes leads to ∼90:10 mixtures of isomeric diene products that can be deprotonated to give simple boryl cyclopentadienides. We extended this transformation to the sterically hindered lithium tert-butylcyclopentadienide 1 using FBMes (Mes = 2,4,6-trimethylphenyl) and ClBCy as electrophiles. The boryl group is selectively introduced in the remote position to minimize steric congestion. The new boryl dienes are obtained as mixtures of isomers, and subsequent deprotonation with MeLi or LiHMDS affords the lithium 1,3-disubstituted cyclopentadienides 5a,b in yields over 95%. Direct assembling of tert-butylated boryl cyclopentadienides with MCl (M = Fe, Co) selectively leads to 1,1'-planar chiral ferrocenes 6a,b and cobaltocene 7. To shed light into the diastereoselective formation of 6a, DFT calculations were performed. The potential energy surface was scrutinized so as to identify and compare its diastereoisomers and conformers. This stereoselectivity is attributed to minimized steric repulsions between the tert-butyl and the BMes groups in the eclipsed conformation of the racemic diastereoisomers. The X-ray structures of boryl diene 2a and diboryl ferrocene 6a are reported. The electronic structure of cobaltocene 7 was analyzed by EPR and DFT calculations. The spin density of this unique open-shell complex is mainly localized on the Co center, but significant spin density is also found on the boron atoms, indicating substantial delocalization of the unpaired electron over the Lewis acid moieties. Consistently, the singly occupied molecular orbital is a combination of a Co-centered 3d orbital with π(BC) orbitals on each CpBMes rings. There is only weak, if any, direct M···B interaction in 6 and 7.
未取代的碱金属环戊二烯化物与卤代硼烷反应生成约90:10的异构二烯产物混合物,这些产物可去质子化得到简单的硼基环戊二烯化物。我们使用FBMes(Mes = 2,4,6 - 三甲基苯基)和ClBCy作为亲电试剂,将这种转化扩展到空间位阻较大的叔丁基环戊二烯基锂1。硼基选择性地引入到较远位置以最小化空间拥挤。新的硼基二烯以异构体混合物形式获得,随后用MeLi或LiHMDS去质子化,以超过95%的产率得到1,3 - 二取代环戊二烯基锂5a,b。叔丁基化硼基环戊二烯化物与MCl(M = Fe, Co)直接组装选择性地生成1,1'-平面手性二茂铁6a,b和钴茂7。为了阐明6a的非对映选择性形成,进行了DFT计算。对势能面进行了仔细研究,以识别和比较其非对映异构体和构象。这种立体选择性归因于外消旋非对映异构体的重叠构象中叔丁基和BMes基团之间的空间排斥最小化。报道了硼基二烯2a和二硼基二茂铁6a的X射线结构。通过EPR和DFT计算分析了钴茂7的电子结构。这种独特的开壳配合物的自旋密度主要定域在Co中心,但在硼原子上也发现了显著的自旋密度,表明未成对电子在路易斯酸部分上有大量离域。一致地,单占据分子轨道是一个以Co为中心的3d轨道与每个CpBMes环上的π(BC)轨道的组合。在6和7中只有微弱的(如果有的话)直接M···B相互作用。