Results and dicussion
The vibrational bands of the E−X transition have been reassigned to the nν3 and ν2+nν3 progressions. [normal modes of C2H2]
The predissociation rates from the D and F Rydberg states are accelerated by the C−H anti-symmetric stretch.
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The level energies and the homogeneous bandwidths, which correspond to the predissociation rates, of the observed vibronic states of acetylene in the D, E, and F states have been determined in the present study. [graph]
Energies of peak positions and their Lorentzian widths. State Assignment Wavenumber
/cm−1Vibrational
energy /cm−1Full width at half
Maximum /cm−1D 0 74490.2(1) 0 58.9(4) 21 76270 a 1780 87 a 31 77629(3) 3139(3) 184(13) 1131 80677(5) 6187(5) 139(19) E 32 74029(1) 1276 b 50(4) 33 74614.5(3) 1861.5 b 26(1) 2131 75011(1) 2258 b 40(4) 34 75243(1) 2490 b 55(5) 2132 75580 2827 b 35 75850 a 3097 b 37 a 2133 76100 a 3347 b 43 a F 0 74751.4(1) 0 66.7(2) 21 76480 a 1729 53 a 31 77817(3) 3066(3) 103(5) 1131 80944(3) 6193(3) 149(14) a P. Löffler et al., Chem. Phys. Lett. 252, 304 (1996); P. Löffler et al., J. Chem. Phys. 109, 5231 (1998)
b The origin band is 72753 cm−1 (Ref. M.N.R. Ashfld et al., J. Chem. Phys. 87, 5105 (1987)
The quantum yield for the production of C2H(A,B) fragment through the D 1Πu Rydnerg state is larger than through the F 1Σu+ Rydberg state.
The predissociation process through the origin of D and F Rydberg states have comparable rates, while that through the E1Avalence state is slower. [graph]