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首页> 外文期刊>The journal of physical chemistry, A. Molecules, spectroscopy, kinetics, environment, & general theory >Internal Methyl Rotation in the CH Stretching Overtone Spectra of Toluene-#alpha#-d_2,-#alpha#-d_1,and -d_0
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Internal Methyl Rotation in the CH Stretching Overtone Spectra of Toluene-#alpha#-d_2,-#alpha#-d_1,and -d_0

机译:甲苯-#alpha#-d_2,-#alpha#-d_1和-d_0的CH拉伸泛音谱中的内部甲基旋转

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摘要

The room-temperature vapor phase spectrum of toluene-#alpha-d_2 has been recorded in the CH stretching region corresponging to triangle open#upsilon#_(CH) = 2-6 with conventional enar-infrared spectroscopy (triangle open#upsilon#_(CH) = 2-4) and with intracavity titanium:sapphire and dye laser photoacoustic spectroscopy (triangle open#upsilon#_(CH) = 2-6). Both absolute oscillator strengths (conventional spectra) and relative oscillator oscillator strengths within a given overtond (conventioal and photoacoustic spectra) have been measured. The aryl region of the spectrum is interpreted interms of two nonequivalent aryl local modes and is essectially identical to the aryl regions of the spectra of toluene-d_0 and toluene-#alpha#-d_1.However,the methyl band profile profile differs significantly in these three molecules.We use an anharmonc oscillator local mode model and an ab initio dipole moment function to calculate oscillator strengths for the aryl and methyl transitions.Parameters for this model come from a fit of the aryl taransition energies and from a fit of the methyl spectral profiles.These simple calculations give values that are in good agreement with observed absolute and relative intensities. Differences in the methyl profiles in toluene-d_0, -#alpha#-d_1,and -#alpha#-d_2 are ascribed to coupling between CH stretching and methyl torsional modes.The methyl profiles are simulatded on the basis of a simple adiabatic model that incorporates the harmonically coupledanharmonic oscillaror local model approach and our intensity calculations.The model successfully accounts for the change in methyl profiles between the three molecules,demonstrates the importance of torsional stretching coupling,and shows that coupling between the CH stretching oscillators is unimportant for higher overtones (triangle open#upsilon#_(CH) >= 4).
机译:甲苯-#alpha-d_2的室温气相色谱已记录在CH拉伸区域中,对应于使用常规的红外光谱的三角形打开#upsilon #_(CH)= 2-6(三角形打开#upsilon#_ (CH)= 2-4)并使用腔内钛:蓝宝石和染料激光光声光谱法(三角形开口#upsilon #_(CH)= 2-6)。在给定的色度内,绝对振荡器强度(常规频谱)和相对振荡器振荡器强度(常规和光声频谱)均已测量。光谱中的芳基区域被解释为两个非等价的芳基局部模式的术语,并且在本质上与甲苯-d_0和甲苯-#α#-d_1的光谱的芳基区域相同。三个分子。我们使用非谐振荡器局部模式模型和从头算起的偶极矩函数来计算芳基和甲基跃迁的振荡器强度,该模型的参数来自芳基tar烷能的拟合以及甲基光谱的拟合这些简单的计算得出的值与观察到的绝对强度和相对强度非常一致。甲苯-d_0,-#alpha#-d_1和-#alpha#-d_2中甲基分布的差异归因于CH拉伸和甲基扭转模式之间的耦合。基于简单的绝热模型模拟甲基分布结合了谐波耦合的非谐振荡器局部模型方法和强度计算。该模型成功地说明了三个分子之间甲基分布的变化,证明了扭转拉伸耦合的重要性,并表明CH拉伸振荡器之间的耦合对于高泛音并不重要。 (三角形open#upsilon #_(CH)> = 4)。

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