Mehn Mark P, Brown Steven D, Jenkins David M, Peters Jonas C, Que Lawrence
Department of Chemistry and Chemical Engineering, Arnold and Mabel Beckman Laboratories of Chemical Synthesis, California Institute of Technology, Pasadena, CA 91125, USA.
Inorg Chem. 2006 Sep 4;45(18):7417-27. doi: 10.1021/ic060670r.
A number of assignments have been previously posited for the metal-nitrogen stretch (nu(M-NR)), the N-R stretch (nu(MN-R)), and possible ligand deformation modes associated with terminally bound imides. Here we examine mononuclear iron(III) and cobalt(III) imido complexes of the monoanionic tridentate ligand [PhBP3] ([PhBP3] = [PhB(CH2PPh2)3]-) to clarify the vibrational features for these trivalent metal imides. We report the structures of [PhBP3]FeNtBu and [PhBP3]CoNtBu. Pseudo-tetrahedral metal imides of these types exhibit short bond lengths (ca. 1.65 A) and nearly linear angles about the M-N-C linkages, indicative of multiple bond character. Furthermore, these compounds give rise to intense, low-energy visible absorptions. Both the position and the intensity of the optical bands in the [PhBP3]MNR complexes depend on whether the substituent is an alkyl or aryl group. Excitation into the low-energy bands of [PhBP3]FeNtBu gives rise to two Raman features at 1104 and 1233 cm(-1), both of which are sensitive to 15N and 2H labeling. The isotope labeling suggests the 1104 cm(-1) mode has the greatest Fe-N stretching character, while the 1233 cm(-1) mode is affected to a lesser extent by (15)N substitution. The spectra of the deuterium-labeled imides further support this assertion. The data demonstrate that the observed peaks are not simple diatomic stretching modes but are extensively coupled to the vibrations of the ancillary organic group. Therefore, describing these complexes as simple diatomic or even triatomic oscillators is an oversimplification. Analogous studies of the corresponding cobalt(III) complex lead to a similar set of isotopically sensitive resonances at 1103 and 1238 cm(-1), corroborating the assignments made in the iron imides. Very minimal changes in the vibrational frequencies are observed upon replacement of cobalt(III) for iron(III), suggesting similar force constants for the two compounds. This is consistent with the previously proposed electronic structure model in which the added electron resides in a relatively nonbonding orbital. Replacement of the tBu group with a phenyl ring leads to a significantly more complicated resonance Raman spectrum, presumably due to coupling with the vibrations of the phenyl ring. Polarization studies demonstrate that the observed modes have A(1) symmetry. In this case, a clearer resonance enhancement of the signals is observed, supporting a charge transfer designation for the electronic transitions. A series of isotope-labeling experiments has been carried out, and the modes with the greatest metal-nitrogen stretching character have been assigned to peaks at approximately 960 and approximately 1300 cm(-1) in both the iron and cobalt [PhBP3]MNPh complexes. These results are consistent with a multiple M-N bond for these metal imides.
此前已对金属 - 氮伸缩振动(ν(M - NR))、N - R伸缩振动(ν(MN - R))以及与末端结合的酰亚胺相关的可能配体变形模式进行了多项研究。在此,我们研究单阴离子三齿配体[PhBP3]([PhBP3] = [PhB(CH2PPh2)3]-)的单核铁(III)和钴(III)酰亚胺配合物,以阐明这些三价金属酰亚胺的振动特征。我们报道了[PhBP3]FeNtBu和[PhBP3]CoNtBu的结构。这类伪四面体金属酰亚胺具有较短的键长(约1.65 Å)以及围绕M - N - C键的近乎线性的角度,这表明存在多重键特征。此外,这些化合物会产生强烈的低能量可见光吸收。[PhBP3]MNR配合物中光学带的位置和强度均取决于取代基是烷基还是芳基。激发[PhBP3]FeNtBu的低能量带会产生两个拉曼特征峰,分别位于1104和1233 cm(-1),这两个峰对15N和2H标记均敏感。同位素标记表明,1104 cm(-1)模式具有最大的Fe - N伸缩特征,而1233 cm(-1)模式受15N取代的影响较小。氘代酰亚胺的光谱进一步支持了这一论断。数据表明,观察到的峰并非简单的双原子伸缩模式,而是与辅助有机基团的振动广泛耦合。因此,将这些配合物描述为简单的双原子甚至三原子振荡器是一种过度简化。对相应钴(III)配合物的类似研究在1103和1238 cm(-1)处产生了一组类似的同位素敏感共振峰,证实了在铁酰亚胺中所做的归属。将钴(III)替换为铁(III)时,观察到振动频率的变化非常微小,这表明这两种化合物具有相似的力常数。这与先前提出的电子结构模型一致,即在该模型中,额外的电子位于相对非键合的轨道中。用苯环取代tBu基团会导致共振拉曼光谱明显更复杂,这可能是由于与苯环的振动耦合所致。偏振研究表明,观察到的模式具有A(1)对称性。在这种情况下,观察到信号有更明显的共振增强,这支持了电子跃迁的电荷转移归属。已进行了一系列同位素标记实验,并且在铁和钴的[PhBP3]MNPh配合物中,具有最大金属 - 氮伸缩特征的模式已被归属于约960和约1300 cm(-1)处的峰。这些结果与这些金属酰亚胺的多重M - N键一致。