首页> 外文期刊>Molecular physics >Rotational analysis of the ν_6, ν_8, ν_3 + ν_4 interacting infrared system of C_2D_6 between 960 cm~(-1) and 1180 cm~(-1)
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Rotational analysis of the ν_6, ν_8, ν_3 + ν_4 interacting infrared system of C_2D_6 between 960 cm~(-1) and 1180 cm~(-1)

机译:C_2D_6在960 cm〜(-1)和1180 cm〜(-1)之间的ν_6,ν_8,ν_3+ν_4相互作用红外系统的旋转分析

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摘要

The Fourier transform infrared spectrum of C_2D_6 (FWHM ≈ 0.0030 cm~(-1)) has been investigated in the region of the ν_6(A_(2u)) and ν_8(E_u) fundamentals, from 960 cm~(-1) to 1180 cm~(-1). A strong x,y Coriolis interaction between ν_6 and ν_8, with K level crossing, generates large displacements of the rotational components of both vibrational states, tuning them to additional local resonances in several spectral regions. Beyond l resonances with Δl = ± 2, Δk = -+1 within ν_8, a z Coriolis-type resonance of ν_3 + ν_(A_(1u)) and ν_6 occurs at K ≤ 6, and an x,y Coriolis-type resonance of ν_8( — l, K— 1) and ν_3 + ν_4(K) occurs at K = 7 and 8. A further coupling of ν_8 (4- /, K— 2) and ν_3 + ν_4(K) has been observed as well. The vibration-rotation constants of ν_6, ν_8 and ν_3 + ν_4, and several interaction parameters, have been determined by the least-squares fit of the available data, with an overall standard deviation σ = 4.6 x 10~(-4) cm~(-1) in the fit of 1661 observed transition wavenumbers. A torsional splitting is observed only in the level ν_8( -l,K=8,J= 20), resonant with 2ν_4 + ν_9( - l, K = 11, J = 20) in which two torsional quanta ν_4 are excited. Many other J components of ν_8(—l,K= 8) are broadened by this interaction. Rules on the symmetries of the allowed perturbing operators and of their torsional components in ethane-like molecules are determined. In the high-barrier limit, we find it useful to factorize the torsional operators into functions of torsional coordinate and momentum operators and trigonometric functions of the torsional angle. Application of these rules to the coupling operators active in this spectrum is made.
机译:在ν_6(A_(2u))和ν_8(E_u)基本面区域,从960 cm〜(-1)到1180,研究了C_2D_6(FWHM≈0.0030 cm〜(-1))的傅立叶变换红外光谱。厘米〜(-1)。 ν_6和ν_8之间的强x,y科里奥利相互作用(具有K水平交叉)会产生两种振动状态的旋转分量的大位移,从而将它们调整到几个光谱区域中的附加局部共振。除了在ν_8内具有Δl=±2,Δk=-+ 1的l个共振之外,在K≤6时发生ν_3+ν_(A_(1_u))和ν_6的z科里奥利型共振,并且x,y的x,y科里奥利型共振ν_8(— l,K-1)和ν_3+ν_4(K)在K = 7和8处发生。另外,还观察到ν_8(4- /,K_2)和ν_3+ν_4(K)的进一步耦合。 。 ν_6,ν_8和ν_3+ν_4的振动旋转常数以及几个相互作用参数由可用数据的最小二乘拟合确定,总体标准偏差σ= 4.6 x 10〜(-4)cm〜 (-1)符合1661年观察到的跃迁波数。仅在水平ν_8(-l,K = 8,J = 20)中观察到扭转分裂,并与2ν_4+ν_9(-l,K = 11,J = 20)共振,其中激发了两个扭转量子ν_4。 ν_8(—l,K = 8)的许多其他J分量通过此相互作用而扩展。确定关于允许的扰动算子及其在乙烷样分子中的扭转分量的对称性的规则。在高障碍物极限中,我们发现将扭转算子分解为扭转坐标和动量算子的函数以及扭转角的三角函数很有用。将这些规则应用于在该频谱中活跃的耦合算子。

著录项

  • 来源
    《Molecular physics》 |1996年第3期|p.663-676|共14页
  • 作者单位

    Dipartimento di Chimica Farmaceutica e Tossicologica, Universita di Napoli, Via D. Montesano 49,I-80131 Napoli, Italy;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 分子物理学;
  • 关键词

  • 入库时间 2022-08-18 01:08:12

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