Universidade de São Paulo, Departamento de Química e Física Molecular, Instituto de Química de São Carlos, São Carlos, SP, Brazil.
Spectrochim Acta A Mol Biomol Spectrosc. 2012 May;90:1-11. doi: 10.1016/j.saa.2012.01.005. Epub 2012 Jan 9.
Some cyanopolyynes, HC(n)N (n=1, 3, …, 17), are investigated by means of calculations at the MP2/cc-pVTZ and CCSD/cc-pVDZ levels. Although the MP2/cc-pVTZ results for geometries and molecular dipole moments are encouraging, the CCSD/cc-pVDZ level was superior for the study of infrared fundamental intensities. The main bands are also analyzed with a charge-charge flux-dipole flux (CCFDF) partition model based on quantities given by the Quantum Theory of Atoms in Molecules (QTAIM). The intensity of vibrations corresponding to the stretching of CH bonds (3471-3473 cm(-1)) increases in line with the number of carbon atoms (from 61 to 146 km mol(-1) between HCN and HC(13)N). This increase is due to the charge flux contribution while the other contributions remain roughly unaltered except for HCN. Moreover, the hydrogen atom loses an almost constant amount of electronic charge during the CH bond enlargement and a small fraction of this charge spreads to atoms farther and farther away from hydrogen as the molecule size increases. The band associated with the doubly degenerate CH bending vibrations (643-732 cm(-1)) presents approximately the same intensity in all the studied cyanopolyynes (from 67 to 76 km mol(-1)). The CCFDF/QTAIM contributions are also nearly the same for these bending modes in HC(5)N and larger systems. The intensity of the mode mostly identified as CN stretching (around 2378-2399 cm(-1) except for HCN) increases from HCN up to HC(7)N (from 0.3 to 83 km mol(-1)) and nearly stabilizes around 80-90 km mol(-1) for larger systems. The CCFDF/QTAIM contributions for this mode also change significantly up to HC(7)N and remain almost constant in larger systems. We also observed the appearing of a very relevant band between 2283 and 2342 cm(-1). This mode is mainly associated with the symmetric stretching of CC triple bonds near the molecule center and exhibits large charge fluxes while the other contributions are almost negligible in the largest cyanopolyynes. The two vibrational bands associated with the smallest frequencies are also studied and extrapolation equations are suggested to predict their positions in larger cyanopolyynes.
一些氰基齐聚物,HC(n)N(n=1、3、…、17),通过 MP2/cc-pVTZ 和 CCSD/cc-pVDZ 水平的计算进行了研究。尽管 MP2/cc-pVTZ 结果在几何形状和分子偶极矩方面令人鼓舞,但 CCSD/cc-pVDZ 水平更适合研究红外基本强度。主要带也通过基于分子中原子量子理论(QTAIM)给出的数量的电荷-电荷通量-偶极通量(CCFDF)分区模型进行了分析。对应于 CH 键拉伸的振动强度(3471-3473cm(-1)) 随着碳原子数的增加而增加(从 HCN 到 HC(13)N,从 61 到 146km mol(-1))。这种增加是由于电荷通量的贡献,而其他贡献除了 HCN 之外基本保持不变。此外,在 CH 键扩大过程中,氢原子失去几乎恒定数量的电子电荷,并且随着分子尺寸的增加,一小部分电荷扩散到离氢原子越来越远的原子上。与双简并 CH 弯曲振动(643-732cm(-1)) 相关的带在所有研究的氰基齐聚物中呈现出大致相同的强度(从 67 到 76km mol(-1))。对于 HC(5)N 和更大的系统,这些弯曲模式的 CCFDF/QTAIM 贡献也几乎相同。主要被识别为 CN 拉伸的模式(除 HCN 外约为 2378-2399cm(-1)) 从 HCN 增加到 HC(7)N(从 0.3 到 83km mol(-1)),并在更大的系统中稳定在 80-90km mol(-1)左右。对于这个模式,CCFDF/QTAIM 贡献也在 HC(7)N 之前发生显著变化,并在更大的系统中保持几乎不变。我们还观察到在 2283 到 2342cm(-1) 之间出现了一个非常相关的带。这个模式主要与分子中心附近 CC 三键的对称拉伸有关,表现出较大的电荷通量,而其他贡献在最大的氰基齐聚物中几乎可以忽略不计。还研究了与最小频率相关的两个振动带,并提出了外推方程以预测它们在更大的氰基齐聚物中的位置。