Department of Applied Chemistry, Faculty of Engineering, Kanagawa Institute of Technology, Atsugi, Kanagawa 240-0292, Japan.
J Phys Chem A. 2012 Feb 2;116(4):1224-36. doi: 10.1021/jp211030h. Epub 2012 Jan 23.
The rotational spectra of the CO-ethylene oxide (EO), CO-ethylene sulfide (ES), CO(2)-EO, and CO(2)-ES complexes were measured by Fourier transform microwave spectroscopy in the frequency region from 4 up to 31 GHz. The isotopologues with a single (13)C atom in the EO or ES, (18)O in the EO, (34)S in the ES, and (13)C in the CO(2) moiety, respectively, were observed in natural abundance, and enriched samples, (13)CO or C(18)O in the CO-EO or CO-ES complex and C(18)OO and C(18)O(2) in the CO(2)-EO or CO(2)-ES complex, were employed to record respective rotational transitions. The rotational spectra observed for the CO-EO, CO-ES, CO(2)-EO, and CO(2)-ES complexes were analyzed by using an asymmetric-rotor S-reduced Hamiltonian to determine rotational and centrifugal distortion constants. The r(s) coordinates of the atoms in the four complexes, which were calculated from the observed rotational constants, led to a structure in which the CO or CO(2) moiety is located in a plane perpendicular to the EO or ES skeletal plane and bisecting the COC or CSC angle. We have also carried out ab initio molecular orbital calculations at the level of MP2 with basis sets 6-311++G(d,p) and aug-cc-pVDZ using the Gaussian 09 package. The MP2/6-311++G(d,p) calculations yield rotational constants in better agreement with the experimental values than with the other basis set; in other words, the molecular structures calculated using this basis set are close to those experimentally found for the ground state. The estimated dissociation energies of the complexes, including the zero-point vibrational energy corrections ΔZPV and the basis set superposition errors (BSSE) calculated with the counterpoise correction (CP), are in good agreement with the experimentally obtained binding energies E(B). We have applied an NBO analysis to the complexes to calculate the stabilization energy CT (=ΔE(σσ*)), which we found are closely correlated with the binding energies E(B). We have thus achieved a consistent overview on the intermolecular interaction in the complexes under consideration. It is to be noted that the spectral intensities of the inner OC(18)O-EO and OC(18)O-ES complexes were larger by a factor of 2 than those of the outer (18)OCO-EO/ES complexes. This observation was explained by the zero-point energy of the inner conformer being a little smaller than that of the outer one.
一氧化碳-氧化乙烯(EO)、一氧化碳-乙硫醚(ES)、二氧化碳-氧化乙烯(EO)和二氧化碳-乙硫醚(ES)复合物的旋转光谱通过傅里叶变换微波光谱法在 4 至 31GHz 的频率范围内进行了测量。在天然丰度和富集样品中观察到了在 EO 或 ES 中具有单个 (13)C 原子、在 EO 中具有 (18)O、在 ES 中具有 (34)S 和在 CO(2)部分中具有 (13)C 的同位素,分别使用 (13)CO 或 C(18)O 在 CO-EO 或 CO-ES 复合物和 C(18)OO 和 C(18)O(2)在 CO(2)-EO 或 CO(2)-ES 复合物中记录各自的转动跃迁。使用非对称转子 S 约化哈密顿量对观察到的 CO-EO、CO-ES、CO(2)-EO 和 CO(2)-ES 复合物的旋转光谱进行了分析,以确定旋转和离心畸变常数。根据观察到的旋转常数计算出四个复合物中原子的 r(s)坐标,导致了一个结构,其中 CO 或 CO(2)部分位于垂直于 EO 或 ES 骨架平面的平面内,并平分 COC 或 CSC 角。我们还使用高斯 09 包在 MP2 水平上使用基组 6-311++G(d,p)和 aug-cc-pVDZ 进行了从头算分子轨道计算。MP2/6-311++G(d,p)计算得到的旋转常数与实验值的一致性优于其他基组;换句话说,使用该基组计算的分子结构与实验上发现的基态分子结构接近。复合物的估计离解能,包括零点振动能校正 ΔZPV 和使用平衡校正(CP)计算的基组叠加误差(BSSE),与实验获得的结合能 E(B)很好地吻合。我们已经将 NBO 分析应用于复合物,以计算稳定化能 CT(=ΔE(σσ*)),我们发现该能量与结合能 E(B)密切相关。因此,我们对所考虑的复合物中的分子间相互作用有了一个一致的概述。需要注意的是,内部 OC(18)O-EO 和 OC(18)O-ES 复合物的光谱强度比外部 (18)OCO-EO/ES 复合物的光谱强度大 2 倍。这一观察结果可以通过内部构象的零点能略小于外部构象的零点能来解释。