Idec Aneta, Pawlicki Miłosz, Latos-Grażyński Lechosław
Department of Chemistry, University of Wrocław , 14 F. Joliot-Curie Street, 50-383 Wrocław, Poland.
Inorg Chem. 2017 Sep 5;56(17):10337-10352. doi: 10.1021/acs.inorgchem.7b01237. Epub 2017 Aug 15.
A diamagnetic ruthenium(II) complex of 5,10,15,20-tetraphenyl-p-benziporphyrin [Ru(p-BzP)(CO)Cl] was obtained via the insertion of ruthenium into p-benziporphyrin using triruthenium(0) dodecacarbonyl [Ru(CO)] as the metal source. The procedure applying dichloro(cycloocta-1,5-diene)ruthenium(II) (polymer, [Ru(COD)Cl]) afforded the paramagnetic six-coordinate ruthenium(III) p-benziporphyrin [Ru(p-BzP)Cl]. As shown by X-ray crystallography, the p-phenylene ring in both complexes is sharply tilted out of the N plane, as reflected by the respective N (pyrrole)-C (p-phenylene) dihedral angle [Ru(p-BzP)(CO)Cl, 52.5°; Ru(p-BzP)Cl, 53.7°]. p-Phenylene is bound to the ruthenium cation in an η fashion, revealing the shortest ever Ru-C distance in the series of p-benziporphyrin complexes [Ru(p-BzP)(CO)Cl, 2.275(2) Å; Ru(p-BzP)Cl, 2.324(5) Å]. The reaction of Ru(p-BzP)(CO)Cl with ArMgCl or AlkMgCl results in the formation of diamagnetic six-coordinate ruthenium(II) p-benziporphyrin complexes containing the apically coordinated σ-alkyl or σ-aryl ligands, where the metal ion simultaneously coordinates to three carbon centers respectively accommodating η (phenylene) and σ (aryl and alkyl) modes. Reactions of σ-aryl (alkyl) carbanions with paramagnetic Ru(p-BzP)Cl have been followed by H NMR spectroscopy. The procedure afforded the six-coordinate paramagnetic ruthenium(III) p-benziporphyrin [Ru(p-BzP)(Ph)Cl], which binds one σ-aryl ligand, as reflected by the characteristic H NMR spectra spread within the +120 to -120 ppm range. Both paramagnetic complexes Ru(p-BzP)(Ph)Cl and Ru(p-BzP)(p-Tol)Cl are formed as a mixture of two stereoisomers differentiated by two nonequivalent locations of σ-aryl with respect to the puckered macrocyclic ring. The paramagnetic shifts of σ-aryls are indicative of π-spin delocalization patterns. Analysis of the contact shifts and parallel density functional theory calculations of the spin density distribution in Ru(p-BzP)Cl, Ru(p-BzP)(Ar)Cl, and Ru(p-BzP)(Alk)Cl reflect the features of the d(dd) electronic ground state.
通过使用十二羰基三钌(0)[Ru₃(CO)₁₂]作为金属源将钌插入对二苯并卟啉中,得到了5,10,15,20-四苯基对二苯并卟啉的抗磁性钌(II)配合物[Ru(p-BzP)(CO)Cl]。采用二氯(环辛-1,5-二烯)钌(II)(聚合物,[Ru(COD)Cl₂])的方法得到了顺磁性的六配位钌(III)对二苯并卟啉[Ru(p-BzP)Cl₂]。X射线晶体学表明,两种配合物中的对亚苯基环都急剧倾斜出N平面,这由各自的N(吡咯)-C(对亚苯基)二面角反映出来[Ru(p-BzP)(CO)Cl,52.5°;Ru(p-BzP)Cl₂,53.7°]。对亚苯基以η方式与钌阳离子结合,揭示了对二苯并卟啉配合物系列中最短的Ru-C距离[Ru(p-BzP)(CO)Cl,2.275(2) Å;Ru(p-BzP)Cl₂,2.324(5) Å]。Ru(p-BzP)(CO)Cl与ArMgCl或AlkMgCl反应生成含有顶端配位的σ-烷基或σ-芳基配体的抗磁性六配位钌(II)对二苯并卟啉配合物,其中金属离子同时分别与三个碳中心配位,分别容纳η(亚苯基)和σ(芳基和烷基)模式。通过¹H NMR光谱跟踪了σ-芳基(烷基)碳负离子与顺磁性Ru(p-BzP)Cl₂的反应。该方法得到了六配位顺磁性钌(III)对二苯并卟啉[Ru(p-BzP)(Ph)Cl₂],它结合了一个σ-芳基配体,这由在+120至-120 ppm范围内扩展的特征¹H NMR光谱反映出来。顺磁性配合物Ru(p-BzP)(Ph)Cl₂和Ru(p-BzP)(p-Tol)Cl₂都是以两种立体异构体的混合物形式形成的,这两种立体异构体由σ-芳基相对于褶皱大环的两个不等价位置区分。σ-芳基的顺磁位移表明了π-自旋离域模式。对Ru(p-BzP)Cl₂、Ru(p-BzP)(Ar)Cl₂和Ru(p-BzP)(Alk)Cl₂中自旋密度分布的接触位移分析和平行密度泛函理论计算反映了d(dd)电子基态的特征。