Department of Molecular Engineering, Graduate School of Engineering, Kyoto University, Nishikyo-ku, Kyoto 615-8510, Japan.
J Phys Chem A. 2010 Jan 21;114(2):1191-9. doi: 10.1021/jp909796h.
Inverted sandwich type chromium(I) complexes, (mu-eta(6):eta(6)-C(6)H(5)CH(3))Cr(DDP) (DDPH = 2-(4-{(2,6-diisopropylphenyl)imino}pent-2-ene) and (mu-eta(6):eta(6)-C(6)H(5)CH(3))V(DDP), synthesized by Tsai et al., and (mu-eta(6):eta(6)-C(6)H(6))Cr(DDP) synthesized by Monillas et al., were theoretically investigated with MRMP2 and DFT methods, where model compounds (mu-eta(6):eta(6)-C(6)H(6))Cr(AIP) (AIPH = (Z)-1-amino-3-imino-prop-1-ene) were mainly employed. Both computational methods succeeded in reproducing the experimental facts that the chromium and vanadium complexes take surprisingly high spin states, septet and quintet spin states, respectively. MO diagrams of these complexes present a clear understanding of the reasons why they take such high spin states. We also calculated their analogues, (mu-eta(6):eta(6)-C(6)H(6))M(DDP) (M = Sc, Ti, Mn, or Fe). The spin multiplicities of the Sc and Ti complexes were calculated to be singlet and triplet, respectively, by the DFT(B3LYP) method. Those of Mn and Fe complexes were calculated to be quintet and triplet, respectively, by the DFT(B3LYP) method, but nonet and singlet, respectively, by the MRMP2 method, suggesting that the DFT method cannot be applied to these complexes. The MRMP2 calculations indicate that the spin multiplicity increases upon going to Mn from Sc and reaches the maximum, nonet spin state, at Mn, and then suddenly decreases to singlet at Fe. This interesting change in spin multiplicity is discussed in terms of occupation of MOs.
反三明治型铬(I)配合物,(mu-eta(6):eta(6)-C(6)H(5)CH(3))Cr(DDP) (DDPH = 2-(4-{(2,6-二异丙基苯基)亚氨基}戊-2-烯)和(mu-eta(6):eta(6)-C(6)H(5)CH(3))V(DDP),由 Tsai 等人合成,以及(mu-eta(6):eta(6)-C(6)H(6))Cr(DDP),由 Monillas 等人合成,用 MRMP2 和 DFT 方法进行了理论研究,其中主要使用模型化合物(mu-eta(6):eta(6)-C(6)H(6))Cr(AIP) (AIPH = (Z)-1-氨基-3-亚氨基丙-1-烯)。这两种计算方法都成功地再现了实验事实,即铬和钒配合物分别采取令人惊讶的高自旋态,七重态和五重态。这些配合物的 MO 图清楚地说明了它们采取如此高自旋态的原因。我们还计算了它们的类似物,(mu-eta(6):eta(6)-C(6)H(6))M(DDP) (M = Sc, Ti, Mn 或 Fe)。DFT(B3LYP)方法计算 Sc 和 Ti 配合物的自旋多重性分别为单重态和三重态。Mn 和 Fe 配合物的自旋多重性分别为五重态和三重态,但 MRMP2 方法计算的分别为九重态和单重态,表明 DFT 方法不适用于这些配合物。MRMP2 计算表明,自旋多重性从 Sc 到 Mn 增加,在 Mn 处达到最大值,九重态,然后在 Fe 处突然降至单重态。这种有趣的自旋多重性变化是根据 MO 的占据情况讨论的。