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2-甲氧基苯基异氰酸酯和 2-甲氧基苯基异硫氰酸酯:构象体、振动结构和多重费米共振。

2-Methoxyphenyl isocyanate and 2-Methoxyphenyl isothiocyanate: conformers, vibration structure and multiplet Fermi resonance.

机构信息

Department of Physics, Karnatak University, Dharwad 580 003, India.

出版信息

Spectrochim Acta A Mol Biomol Spectrosc. 2012 Jun;91:261-8. doi: 10.1016/j.saa.2012.01.024. Epub 2012 Feb 8.

DOI:10.1016/j.saa.2012.01.024
PMID:22381801
Abstract

IR and Raman spectral measurements in the region 3500-400/50 cm(-1) have been made for the liquid samples of 2-Methoxyphenyl isocyanate and 2-Methoxyphenyl isothiocyanate. A complete assignment of the measured bands has been proposed as aided by conformational and vibration analyses at B3LYP/6-311++G** level of calculations. Three conformers for 2-Methoxyphenyl isocyanate and two for 2-Methoxyphenyl isothiocyanate have been determined. The tilt of the isocyanate (NCO) and isothiocyanate (NCS) moieties with respect to phenyl ring are in broad agreement with their parents. Stretching mode frequencies of methyl group (-OCH(3)) in 2-Methoxyphenyl isocyanate have been lowered in the 2900-2800 cm(-1); deformation asymmetric modes are IR strong and symmetric one Raman strong. In 2-Methoxyphenyl isothiocyanate, a similar pattern is true for stretching modes but deformation asymmetric modes are IR strong and symmetric mode has not been observed. Multiplet absorption band system near 2200 cm(-1) in 2-Methoxyphenyl isocyanate has been interpreted to be caused by Fermi resonance. A similar pattern in absorption near 2100 cm(-1) in 2-Methoxyphenyl isothiocyanate but more complex Raman band pattern has also been explained through Fermi resonance from heuristic stand-point. Many Raman modes in 1300-1100 cm(-1) are intensified apparently owing to isothiocyanate than isocyanate moiety. Phenyl ring breathing mode is shifted to 1040 cm(-1) as strong Raman; the symmetric stretching mode of O-CH(3) near 1023 cm(-1) as strong absorption.

摘要

已对 2-甲氧基苯基异氰酸酯和 2-甲氧基苯基异硫氰酸酯的液体样品在 3500-400/50 cm(-1) 区域进行了红外和拉曼光谱测量。在 B3LYP/6-311++G** 计算水平的构象和振动分析的辅助下,提出了对测量带的完整分配。确定了 2-甲氧基苯基异氰酸酯的三个构象和 2-甲氧基苯基异硫氰酸酯的两个构象。异氰酸酯(NCO)和异硫氰酸酯(NCS)部分相对于苯基环的倾斜度与它们的母体大致一致。2-甲氧基苯基异氰酸酯中甲基(-OCH(3))的伸缩模式频率在 2900-2800 cm(-1) 范围内降低;变形不对称模式在红外中是强的,而对称模式在拉曼中是强的。在 2-甲氧基苯基异硫氰酸酯中,类似的模式适用于伸缩模式,但变形不对称模式在红外中是强的,而对称模式没有被观察到。2-甲氧基苯基异氰酸酯中近 2200 cm(-1) 的多峰吸收带系统被解释为费米共振引起的。在 2-甲氧基苯基异硫氰酸酯中近 2100 cm(-1) 的吸收也有类似的模式,但更复杂的拉曼带模式也从启发式的角度通过费米共振来解释。由于异硫氰酸酯部分,1300-1100 cm(-1) 处的许多拉曼模式明显增强。苯环呼吸模式移至 1040 cm(-1) 处,为强拉曼;O-CH(3)的对称伸缩模式在 1023 cm(-1) 附近,为强吸收。

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