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Infrared vibrational spectroscopy of cis-dichloroethene in Rydberg states

机译:Rydberg州的顺式-二氯乙烯的红外振动光谱

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We have measured the infrared (IR) vibrational spectrum for cis-dichloroethene (cis-ClCH = CHCl) in excited Rydberg states with the effective principal quantum numbers n(*)=9, 13, 17, 21, 28, and 55 using the vacuum ultraviolet-IR-photoinduced Rydberg ionization (VUV-IR-PIRI) scheme. Although the IR frequencies observed for the vibrational bands nu(11)(*) (asymmetric C-H stretch) and nu(12)(*) (symmetric C-H stretch) are essentially unchanged for different n(*) states, suggesting that the IR absorption predominantly involves the ion core and that the Rydberg electron behaves as a spectator; the intensity ratio for the nu(11)(*) and nu(12)(*) bands [R(nu(11)(*)u(12)(*))] is found to decrease smoothly as n(*) is increased. This trend is consistent with the results of a model ab initio quantum calculation of R(nu(11)(*)u(12)(*)) for excited cis-ClCH = CHCl in n(*)=3-18 states and the MP2/6-311++G(2df,p) calculations of R(nu(11)u(12)) and R(nu(11)(+)u(12)(+)), where R(nu(11)u(12))[R(nu(11)(+)u(12)(+))] represents the intensity ratio of the nu(11)(nu(11)(+)) asymmetric C-H stretching to the nu(12)(nu(12)(+)) symmetric C-H stretching vibrational bands for cis-ClCH = CHCl (cis-ClCH = CHCl+). We have also measured the IR-VUV-photoion (IR-VUV-PI) and IR-VUV-pulsed field ionization-photoelectron depletion (IR-VUV-PFI-PED) spectra for cis-ClCH = CHCl. These spectra are consistent with ab initio calculations, indicating that the IR absorption cross section for the nu(12) band is negligibly small compared to that for the nu(11) band. While the VUV-IR-PIRI measurements have allowed the determination of nu(11)(+)=3067 +/- 2 cm(-1), nu(12)(+)=3090 +/- 2 cm(-1), and R(nu(11)(+)u(12)(+))approximate to 1.3 for cis-ClCH = CHCl+, the IR-VUV-PI and IR-VUV-PFI-PED measurements have provided the value nu(11)=3088.5 +/- 0.2 cm(-1) for cis-ClCH = CHCl.
机译:我们已经使用有效的主量子数n(*)= 9、13、17、21、28和55测量了在激发的里德堡态下的顺式二氯乙烯(cis-ClCH = CHCl)的红外(IR)振动光谱。真空紫外红外光诱导的里德堡电离(VUV-IR-PIRI)方案。虽然观察到的振动带nu(11)(*)(不对称CH拉伸)和nu(12)(*)(对称CH拉伸)的红外频率对于不同的n(*)状态基本上没有变化,这表明红外吸收主要涉及离子核,并且里德堡电子表现为一个旁观者;发现nu(11)(*)和nu(12)(*)波段的强度比[R(nu(11)(*)/ nu(12)(*))]随着n(* )增加。此趋势与在n(*)= 3-18状态下激发的顺式ClCH = CHCl的R(nu(11)(*)/ nu(12)(*))的模型从头量子计算的结果一致以及R(nu(11)/ nu(12))和R(nu(11)(+)/ nu(12)(+))的MP2 / 6-311 ++ G(2df,p)计算,其中R(nu(11)/ nu(12))[R(nu(11)(+)/ nu(12)(+))]表示nu(11)(nu(11)(+)的强度比)将不对称CH拉伸至nu(12)(nu(12)(+))对称CH拉伸振动带,适用于cis-ClCH = CHCl(cis-ClCH = CHCl +)。我们还测量了顺-ClCH = CHCl的IR-VUV-光电离(IR-VUV-PI)和IR-VUV脉冲场电离-光电子耗竭(IR-VUV-PFI-PED)光谱。这些光谱与从头算相符,表明nu(12)波段的红外吸收截面与nu(11)波段的红外吸收截面相比可以忽略不计。虽然VUV-IR-PIRI测量允许确定nu(11)(+)= 3067 +/- 2 cm(-1),但nu(12)(+)= 3090 +/- 2 cm(-1) ,并且对于cis-ClCH = CHCl +,R(nu(11)(+)/ nu(12)(+))大约为1.3,IR-VUV-PI和IR-VUV-PFI-PED测量提供了值nu (11)= 3088.5 +/- 0.2 cm(-1)对于顺式ClCH = CHCl。

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