Department of Chemistry, Faculty of Science, Ochanomizu University, 2-1-1 Otsuka, Bunkyo-ku, Tokyo 112-8610, Japan.
J Chem Phys. 2012 Dec 28;137(24):244303. doi: 10.1063/1.4769283.
FeCO is a molecule of astrophysical interest. We report here theoretical calculations of its geometrical parameters, electronic structures, and molecular constants (such as dipole moment and spin-orbit coupling constant) in the electronic ground state X(3)Σ(-) and the low-lying triplet and quintet excited states. The calculations were made at the MR-SDCI+Q_DK3/[5ZP ANO-RCC (Fe, C, O)] and MR-AQCC_DK3/[5ZP ANO-RCC (Fe, C, O)] levels of theory. A multi-reference calculation was required to describe correctly the wavefunctions of all states studied. For all triplet states, the σ-donation through the 10σ molecular orbital (MO) as well as the π-back-donation through the 4π MO are observed, and the dipole moment vector points from O toward Fe as expected. However, in the excited quintet states (5)Π, (5)Φ, and (5)Δ, the almost negligible contribution of Fe 4s to the 10σ MO makes the dipole moment vector point from Fe toward O, i.e., in the same direction as in CO. In the X(3)Σ(-) state, the electron provided by the σ-donation through the 10σ MO is shared between the Fe atom and the C end of the CO residue to form a coordinate-covalent Fe-C bond. In the ã(5)Σ(-) state (the high-spin counterpart of X(3)Σ(-)), the σ-donation through the 10σ MO is not significant and so the Fe-C bond is rather ionic. The π-back-donation through the 4π MO is found to be of comparable importance in the two electronic states; it has a slightly larger magnitude in the X(3)Σ(-) state. The difference in the molecular properties of the low-spin X(3)Σ(-) and the high-spin ã(5)Σ(-) states can be understood in terms of the dynamical electron correlation effects.
FeCO 是一种天体物理感兴趣的分子。我们在这里报告其电子基态 X(3)Σ(-)和低能三重态和五重态激发态的几何参数、电子结构和分子常数(如偶极矩和自旋-轨道耦合常数)的理论计算。计算是在 MR-SDCI+Q_DK3/[5ZP ANO-RCC (Fe, C, O)] 和 MR-AQCC_DK3/[5ZP ANO-RCC (Fe, C, O)]理论水平上进行的。需要进行多参考计算才能正确描述所有研究状态的波函数。对于所有三重态,观察到通过 10σ分子轨道(MO)的σ供体以及通过 4π MO 的π反向供体,偶极矩向量指向预期的 Fe 向 O。然而,在激发的五重态(5)Π、(5)Φ 和(5)Δ中,Fe 4s 对 10σ MO 的几乎可以忽略不计的贡献使得偶极矩向量指向 O,即与 CO 中的方向相同。在 X(3)Σ(-)态中,通过 10σ MO 的σ供体提供的电子被 Fe 原子和 CO 残基的 C 端共享,形成配位共价 Fe-C 键。在ã(5)Σ(-)态(X(3)Σ(-)的高自旋对应态)中,通过 10σ MO 的σ供体不重要,因此 Fe-C 键是离子的。通过 4π MO 的π反向供体在两个电子态中具有相当的重要性;在 X(3)Σ(-)态中,其幅度略大。低自旋 X(3)Σ(-)和高自旋ã(5)Σ(-)态的分子性质的差异可以用动态电子相关效应来理解。