首页> 外文期刊>Journal of Molecular Spectroscopy >10 μm High-resolution spectrum of trans-acrolein: Rotational analysis of the ν_(11), ν_(16), ν_(14) and ν_(16) + ν_(18) - ν_(18) bands
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10 μm High-resolution spectrum of trans-acrolein: Rotational analysis of the ν_(11), ν_(16), ν_(14) and ν_(16) + ν_(18) - ν_(18) bands

机译:10μm反式丙烯醛的高分辨率光谱:ν_(11),ν_(16),ν_(14)和ν_(16)+ν_(18)-ν_(18)谱带的旋转分析

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High-resolution Fourier transform spectra of trans-acrolein, H _2CC(H)C(H)O, have been recorded in the 10 μm region at both room and cooled temperatures on the modified Bomem DA3.002 at the National Research Council of Canada and the Bruker IFS 125HR spectrometer at the far infrared beam line of the Canadian Light Source in Saskatoon. Vibrational fundamentals analyzed so far include the ν_(11), ν_(16) and ν_(14) bands centered at 911.3, 958.7 and 992.7 cm~(-1) corresponding respectively to the A′ in-plane CH_2~-rocking mode, the A″ out-of-plane CH_2~-wagging mode, and the A″ wagging mode highly mixed between the ≥CH vinyl and ≥CH formyl groups [Vibrational mode descriptions are based on Y.N. Panchenko, P. Pulay, F. T?r?k, J. Mol. Spectrosc. 34 (1976) 283-289.] As well, the ν_(16) + ν_(18) - ν_(18) hot band centred at 957.6 cm~(-1) has been analyzed, where ν18 is the low-frequency (157.9 cm~(-1)) A″ ≥CC torsional mode. The ν_(11) band is a/b type while the ν_(16), ν_(14) and ν_(16) + ν_(18) - ν_(18) bands are c-type. The assigned transitions of each band have been fitted to a Watson asymmetric rotor Hamiltonian, with ground state parameters fixed to values obtained from rotational analyses in the literature. As well, a combined 3-state fit for ν_(11), ν_(16) and ν_(14) was carried out including Coriolis and Z_1 constants which account for J and ΔK interactions. Transition dipole moments have been calculated for each of the fundamentals using the ab initio B3LYP method and 6-311++G basis set. For the A′ vibrational modes, we have also evaluated transition dipole a- and b-components in the principal axis system from vibrational displacements and dipole moment derivatives. Our ab initio results predict that the ν-(11) in-plane CH_2 rocking mode has an a-type transition strength about three times greater than the b-type, which is consistent with our observations. Our ab initio force field analysis gives vibrational mode descriptions consistent with previously published work for all 13 A′ modes. However, for the five A″ vibrational modes, our ab initio results disagree with two of the descriptions of Panchenko et al. and three of the descriptions of Hamada et al. [Y. Hamada, Y. Nishimura, M. Tsuboi, Chem. Phys. 100 (1985) 365-375].
机译:加拿大国家研究委员会在改良的Bomem DA3.002上在室温和冷却温度下都在10μm区域记录了反丙烯醛H _2CC(H)C(H)O的高分辨率傅里叶变换光谱和位于萨斯卡通的加拿大光源的远红外光束线上的布鲁克IFS 125HR光谱仪。到目前为止分析的振动基本原理包括分别位于911.3、958.7和992.7 cm〜(-1)中心的ν_(11),ν_(16)和ν_(14)谱带,分别对应于A'平面CH_2〜摇摆模式, A“面外CH_2〜摆动模式,并且在≥CH乙烯基和≥CH甲酰基之间高度混合的A”摆动模式[振动模式说明基于YN Panchenko,P.Pulay,F.T?r?k,J.Mol。光谱。 [34(1976)283-289。]也分析了以957.6 cm〜(-1)为中心的ν_(16)+ν_(18)-ν_(18)热带,其中ν18是低频( 157.9 cm〜(-1))A''≥CC扭转模式ν_(11)带是a / b型,而ν_(16),ν_(14)和ν_(16)+ν_(18)-ν_(18)带是c型。每个频带的指定过渡已拟合到Watson非对称转子哈密顿量,其基态参数固定为从文献中的旋转分析获得的值。同样,对ν_(11),ν_(16)和ν_(14)进行了组合的三态拟合,包括考虑到J和ΔK相互作用的科里奥利常数和Z_1常数。已经使用从头算B3LYP方法和6-311 ++ G基集为每个基础计算了跃迁偶极矩。对于A'振动模式,我们还根据振动位移和偶极矩导数评估了主轴系统中的过渡偶极a和b分量。我们的从头算结果预测,v-(11)面内CH_2摇摆模式的a型过渡强度约为b型的三倍,这与我们的观察结果一致。我们的从头算力场分析给出了与所有13种A'模式的振动模式描述相一致的描述。但是,对于五个A''振动模式,我们的从头算结果与Panchenko等人的两个描述不一致。和Hamada等人的三个描述。 [是的。滨田Y.西村,M。Tsuboi,化学。物理100(1985)365-375]。

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