The electronically excited doublet and quartet states of the linear (D ∞h ) and cyclic (C 2V ) C 6 + ion were studied using high-level ab initio methods. For the linear ion it is found that the three lowest excited 2 π g states, which contribute to the n 2 π g -X 2 π u transitions between 1.88 and 2.73 eV, are strongly coupled and form avoided crossings if the bond distances are varied. This leads to a centrosymmetric double minimum potential of the 2 2 π g state. For the cyclic C 2v structures the lowest states have 2 A 1 and 2 B 2 symmetries. At their equilibrium geometries both states are almost degenerate and their energies are 0.3 eV lower than the minimum of the linear X 2 π u state. The excitation energies are strongly affected by geometry relaxation effects. The adiabatic excitation energies of the cyclic 2 2 A 1 and the linear 1 2 π g states are predicted to be about 1.9 eV, i.e. close to the observed band origin. Several electronically excited states-2 2 A 2 , 2 2 B 1 , 2 2 B 2 -of the cyclic structure and the 2 2 π g state of the linear structure were calculated between 2.3 and 2.5eV, i.e. higher than the observed band origin at 2.17eV. Due to strong electronic and vibronic couplings a reliable prediction of relative intensities is presently not possible, and therefore the calculated transition moments cannot be used for the interpretation of the experimental spectrum.
%0 Journal Article
%1 publ9344953
%A Gillery, Claire
%A Rosmus, Pavel
%A Werner, Hans Joachim
%A Stoll, Hermann
%A Maier, John P.
%D 2004
%J Mol. Phys.
%K chemie imported werner from:alexanderdenzel theoretische stuttgart theochem
%N 21-22
%P 2227–2236
%R 10.1080/00268970410001734314
%T A theoretical study of the electronically excited states in linear and cyclic C₆⁺
%U http://dx.doi.org/10.1080/00268970410001734314
%V 102
%X The electronically excited doublet and quartet states of the linear (D ∞h ) and cyclic (C 2V ) C 6 + ion were studied using high-level ab initio methods. For the linear ion it is found that the three lowest excited 2 π g states, which contribute to the n 2 π g -X 2 π u transitions between 1.88 and 2.73 eV, are strongly coupled and form avoided crossings if the bond distances are varied. This leads to a centrosymmetric double minimum potential of the 2 2 π g state. For the cyclic C 2v structures the lowest states have 2 A 1 and 2 B 2 symmetries. At their equilibrium geometries both states are almost degenerate and their energies are 0.3 eV lower than the minimum of the linear X 2 π u state. The excitation energies are strongly affected by geometry relaxation effects. The adiabatic excitation energies of the cyclic 2 2 A 1 and the linear 1 2 π g states are predicted to be about 1.9 eV, i.e. close to the observed band origin. Several electronically excited states-2 2 A 2 , 2 2 B 1 , 2 2 B 2 -of the cyclic structure and the 2 2 π g state of the linear structure were calculated between 2.3 and 2.5eV, i.e. higher than the observed band origin at 2.17eV. Due to strong electronic and vibronic couplings a reliable prediction of relative intensities is presently not possible, and therefore the calculated transition moments cannot be used for the interpretation of the experimental spectrum.
@article{publ9344953,
abstract = {The electronically excited doublet and quartet states of the linear (D ∞h ) and cyclic (C 2V ) C 6 + ion were studied using high-level ab initio methods. For the linear ion it is found that the three lowest excited 2 π g states, which contribute to the n 2 π g -X 2 π u transitions between 1.88 and 2.73 eV, are strongly coupled and form avoided crossings if the bond distances are varied. This leads to a centrosymmetric double minimum potential of the 2 2 π g state. For the cyclic C 2v structures the lowest states have 2 A 1 and 2 B 2 symmetries. At their equilibrium geometries both states are almost degenerate and their energies are 0.3 eV lower than the minimum of the linear X 2 π u state. The excitation energies are strongly affected by geometry relaxation effects. The adiabatic excitation energies of the cyclic 2 2 A 1 and the linear 1 2 π g states are predicted to be about 1.9 eV, i.e. close to the observed band origin. Several electronically excited states-2 2 A 2 , 2 2 B 1 , 2 2 B 2 -of the cyclic structure and the 2 2 π g state of the linear structure were calculated between 2.3 and 2.5eV, i.e. higher than the observed band origin at 2.17eV. Due to strong electronic and vibronic couplings a reliable prediction of relative intensities is presently not possible, and therefore the calculated transition moments cannot be used for the interpretation of the experimental spectrum.},
added-at = {2019-03-01T15:49:43.000+0100},
author = {Gillery, Claire and Rosmus, Pavel and Werner, Hans Joachim and Stoll, Hermann and Maier, John P.},
biburl = {https://puma.ub.uni-stuttgart.de/bibtex/2b70363f8bf6d17f64000bc03aa6d4e13/theochem},
doi = {10.1080/00268970410001734314},
interhash = {aac1e48a39e33be16aba570678e36c74},
intrahash = {b70363f8bf6d17f64000bc03aa6d4e13},
issn = {00268976},
journal = {Mol. Phys.},
keywords = {chemie imported werner from:alexanderdenzel theoretische stuttgart theochem},
number = {21-22},
pages = {2227–2236},
timestamp = {2019-03-01T14:49:43.000+0100},
title = {{A theoretical study of the electronically excited states in linear and cyclic C₆⁺}},
url = {http://dx.doi.org/10.1080/00268970410001734314},
volume = 102,
year = 2004
}