Department of Inorganic and Physical Chemistry, Indian Institute of Science, Bangalore 560012, India.
J Phys Chem A. 2012 Jun 21;116(24):5769-78. doi: 10.1021/jp2045542. Epub 2011 Jul 28.
Infrared spectra of atmospherically and astronomically important dimethylphenanthrenes (DMPs), namely 1,9-DMP, 2,4-DMP, and 3,9-DMP, were recorded in the gas phase from 400 to 4000 cm(-1) with a resolution of 0.5 cm(-1) at 110 °C using a 7.2 m gas cell. DFT calculations at the B3LYP/6-311G** level were carried out to get the harmonic and anharmonic frequencies and their corresponding intensities for the assignment of the observed bands. However, spectral assignments could not be made unambiguously using anharmonic or selectively scaled harmonic frequencies. Therefore, the scaled quantum mechanical (SQM) force field analysis method was adopted to achieve more accurate assignments. In this method force fields instead of frequencies were scaled. The cartesian force field matrix obtained from the gaussian calculations was converted to a nonredundant local coordinate force field matrix and then the force fields were scaled to match experimental frequencies in a consistent manner using a modified version of the UMAT program of the QCPE package. Potential energy distributions (PEDs) of the normal modes in terms of nonredundant local coordinates obtained from these calculations helped us derive the nature of the vibration at each frequency. The intensity of observed bands in the experimental spectra was calculated using estimated vapor pressures of the DMPs. An error analysis of the mean deviation between experimental and calculated intensities reveal that the observed methyl C-H stretching intensity deviates more compared to the aromatic C-H and non C-H stretching bands.
在 110°C 下,使用 7.2 m 长的气室,以 0.5 cm(-1)的分辨率,从 400 到 4000 cm(-1)记录了具有大气和天文重要性的二甲基菲(DMP)的红外光谱,即 1,9-DMP、2,4-DMP 和 3,9-DMP。在 B3LYP/6-311G**水平上进行了 DFT 计算,以获得观察到的带的谐波和非谐波频率及其相应的强度,用于分配。然而,使用非谐波或选择性缩放的谐波频率不能明确地进行光谱分配。因此,采用了标度量子力学(SQM)力场分析方法来实现更准确的分配。在这种方法中,力场而不是频率被缩放。从高斯计算中获得的笛卡尔力场矩阵被转换为非冗余局部坐标力场矩阵,然后使用 QCPE 包的 UMAT 程序的修改版本以一致的方式缩放力场,以匹配实验频率。从这些计算中获得的非冗余局部坐标的正则模式的势能分布(PED)帮助我们得出每个频率处振动的性质。使用 DMP 的估计蒸气压计算实验光谱中观察到的带的强度。实验和计算强度之间的平均偏差的误差分析表明,与芳族 C-H 和非 C-H 伸缩带相比,观察到的甲基 C-H 伸缩强度偏差更大。