Vacuum–ultraviolet absorption and fluorescence spectroscopy of CF2H2, CF2Cl2, and CF2Br2 in the range 8–22 eV

Abstract

The vacuum-UV absorption and fluorescence spectroscopy of CF 2 X 2 (X=H,Cl,Br) in the range nm is reported. Tunable vacuum-UV radiation in the range 8-22 eV from synchrotron sources at either Daresbury, UK or BESSY1, Germany is used to excite the titled molecules. Fluorescence excitation spectra, with undispersed detection of the fluorescence, were recorded at Daresbury with a resolution of 0.1 nm. VUV absorption spectra at a resolution of 0.08 nm, and dispersed emission spectra with an optical resolution of 8 nm were recorded at BESSY1. Action spectra, in which the VUV energy is scanned with detection of the fluorescence at a specific wavelength, were also recorded at BESSY1 with a resolution of 0.3 nm ; appearance energies for production of a particular emitting state of a fragment are then obtained. Using the single-bunch mode of BESSY1, lifetimes of all emitting states that fall in the range ca. 3-80 ns have been measured. The peaks in the VUV absorption spectra of CF 2 X 2 are assigned to Rydberg transitions. For CF 2 H 2 below 11 eV, there is good agreement between the absorption and the fluorescence excitation spectra, whereas above 11 eV and for the whole range 8-22 eV for CF 2 Cl 2 and CF 2 Br 2 there is little similarity. This suggests that photodissociation to emitting states of fragment species represent minor channels. In the range 8-15 eV, emission is due mainly to CF 2 Ã 1 B 1 − X 1 A 1 and weakly to CFX Ã 1 A" − X 1 A'. These products form by photodissociation of Rydberg states of CF 2 X 2 , and the thresholds for their production therefore relate to energies of the Rydberg states of the parent molecule. For CF 2 H 2 below 11.8 eV CF 2 Ã 1 B 1 can only form with H 2 , whereas for CF 2 Cl 2 and CF 2 Br 2 it is not possible to say whether the other products are 2X or X 2 . For energies above ca. 15 eV, emission is due to diatomic fragments ; CF B 2 ∆ and A 2 Σ + , CCl A 2 ∆, CH B 2 Σ -and A 2 ∆, Cl 2 and Br 2 D' 2 3 Π g , and possibly CBr A 2 ∆. From their appearance energies, there is evidence that, with the exception of CF B 2 ∆ / CF 2 H 2 where the ground state of HF must form , the excited state of CF, CCl or CH forms in association with three atoms. Our results yield no information whether the three bonds in CF 2 X 2 * break simultaneously or sequentially. We suggest that the anomalous behaviour of CF 2 H 2 , in forming H-H or H-F bonds in unimolecular photofragmentation processes, relates to the small size of the hydrogen atom, and hence the unimportance of steric effects in the tightlyconstrained transition state. In no cases is emission observed from excited states of either the CF 2 X free radical or the parent molecular ion, CF 2 X 2 + .4

Ion-pair formation mechanisms in chloromethane, bromomethane and dichlorodifluoromethane

“…The assignments of the principal features have been taken from [37] and are included in figure 5. In some cases, these assignments do not match those proposed by Seccombe et al [38] but the differences are not relevant to the present work.…”

Electronic properties and primary dissociation channels of fluoromethane compounds

“…The calculated VUV spectrum using EOMCCSD/aug-cc-pVTZ + 4s + 4p in the energy range of 8-13 eV is shown in Fig. 16, compared with the observed VUV spectrum by Seccombe et al 40) The peak maximum (9.6 eV) of the calculated first band is slightly higher than the observed one (9.2 eV). This may be due to the excited-state potential curves.…”

“…[31][32][33] However, the hydrofluorocarbon gas chemistries, as exemplified by CH 2 F 2 , are representative of fragments such as CHF, CH 2 F, and CHF 2 , leading to differences in etching performance for SiN. [34][35][36][37][38] VUV absorption spectroscopy of CH 2 F 2 in the range of 60-145 nm was reported by Sauvageau et al 39) and absorption and fluorescence spectroscopy of CF 2 F 2 in the range of 190-690 nm was reported by Seccombe et al 40) They reported the first band (peak value of 9.28 eV) and fourth band (peak value of 12.38 eV) are structureless. In the latter report, excited to the first band with a peak value of 9.28 eV, emission due to the CF 2 1 B 1 -1 A 1 transition was observed.…”

The ionic states of difluoromethane: A reappraisal of the low energy photoelectron spectrum including ab initio configuration interaction computations

“…Our ionization energy (IE) range is 12-20 eV. A variety of fragmentation processes [4][5][6][7][8][9][10] compete with direct ionization within that range although these degradations are not expected to be visible in conventional photoelectron spectra. These processes have been summarised in threshold photoelectronphotoion coincidence (TPEPICO) studies 6 on the dissociation of CH 2 F 2 + .…”