Abstract

The vacuum UV photoabsorption spectrum of 1,1-C2H2Cl2 is presented and discussed in detail in the 6–20 eV photon energy range. The broad band observed at 6.488 eV includes the 2b1(π) → σ*, 2b1(π) → π* valence transitions and the 2b1(π) → 3s Rydberg transitions. A quantum chemical calculation analysis is proposed and applied to the intertwined vibrational structure belonging to these transitions. For the π → σ* and π → π* transitions short vibrational progressions are observed, analyzed and tentatively assigned. The π → 3s Rydberg transition is characterized by a single progression starting at 6.746 eV. The fine structure observed between 7.5 and 10.1 eV has been analyzed in terms of vibronic transitions to ns- (δ = 0.89), np- (δ = 0.59 and 0.37) and nd-type (δ = 0.16) Rydberg states all converging to the 1,1-C2H2Cl2+(2B1) ionic ground state. The vibrational structure analysis excitation leads to the following wavenumbers: ω2 ≈ 1310 cm−1 (162 meV), ω4 ≈ 650 cm−1 (81 meV) and ω5 ≈ 290 cm−1 (37 meV). These modes can be assigned to the C=C stretching, to the symmetric C–Cl stretching and to the symmetric Cl–C–Cl bending vibrations respectively. By the same way, eight other Rydberg states were analyzed. For the first time the vacuum UV spectrum of 1,1-C2H2Cl2 has been recorded in the 10–20 eV range, revealing intense broad bands which are assigned to transitions to Rydberg states converging to excited states of 1,1-C2H2Cl2+. Assignments are also proposed for the vibrational excitations observed in this range.

Highlights

  • Further to their wide interest in many fields of both pure and applied chemistry, we initiated a few years ago the systematic investigation of ethylene and its halogenated derivatives

  • For the first time the vacuum UV spectrum of 1,1-C2H2Cl2 has been recorded in the 10–20 eV range, revealing intense broad bands which are assigned to transitions to Rydberg states converging to excited states of 1,1-C2H2Cl2+

  • The vacuum UV photoabsorption spectrum (PAS) of 1,1-C2H2Cl2 between 5 and 15 eV photon energy is represented in figure 1 in terms of the absorbance log10[I0/I] as a function of the photon energy hν

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Summary

Introduction

Further to their wide interest in many fields of both pure and applied chemistry, we initiated a few years ago the systematic investigation of ethylene and its halogenated derivatives. The results about the monosubstituted C2H3X (X = F, Cl and Br) have been reported [1]. The influence of the nature of the substituent on the properties of the neutral (valence and Rydberg) states and the cationic states were discussed in detail. Following an early study of the three C2H2FCl isomers [2] by vacuum UV photoabsorption and photoelectron spectroscopy we reported a detailed investigation of the 1,1-C2H2F2 molecular system by the same techniques [3]. With respect to C2H3F [1] and 1,1-C2H2FCl [2, 4] substitutional effects were observed on, e.g., the π → π* transition whereas the 3s-Rydberg transition energy remains almost unaffected

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