TY - JOUR
T1 - Change in resonance parameters of a linear molecule as it bends: Evidence in electron-impact vibrational transitions of hot COS and CO2 molecules
AU - Hoshino, Masamitsu
AU - Ishijima, Yohei
AU - Kato, Hidetoshi
AU - Mogi, Daisuke
AU - Takahashi, Yoshinao
AU - Fukae, Katsuya
AU - Limão-Vieira, Paulo
AU - Tanaka, Hiroshi
AU - Shimamura, Isao
N1 - This work was conducted under the support of the Japanese Ministry of Education, Culture, Sport, Science and Technology. HK was supported by Grant-in-Aid for JSPS, Grant Number 205032. PLV acknowledges the Portuguese National Funding Agency FCT through research grants PTDC/FIS-ATO/1832/2012 and UID/FIS/00068/2013. PLV also acknowledges his Visiting Professor position at Sophia University, Tokyo, Japan.
PY - 2016/5/3
Y1 - 2016/5/3
N2 - Inelastic and superelastic electron-impact vibrational excitation functions of hot carbonyl sulphide COS (and hot CO2) are measured for electron energies from 0.5 to 3.0 eV (1.5 to 6.0 eV) and at a scattering angle of 90° . Based on the vibrational populations and the principle of detailed balance, these excitation functions are decomposed into contributions from state-to-state vibrational transitions involving up to the second bending overtone (030) in the electronically ground state. Both the2 Π resonance for COS around 1.2 eV and the2 Πu resonance for CO2 around 3.8 eV are shifted to lower energies as the initial vibrational state is excited in the bending mode. The width of the resonance hump for COS changes only little as the molecule bends, whereas that of the overall boomerang resonance for CO2 becomes narrower. The angular distribution of the electrons resonantly scattered by hot COS and hot CO2 is also measured. The different shapes depending on the vibrational transitions and gas temperatures are discussed in terms of the symmetry of the vibrational wave functions.
AB - Inelastic and superelastic electron-impact vibrational excitation functions of hot carbonyl sulphide COS (and hot CO2) are measured for electron energies from 0.5 to 3.0 eV (1.5 to 6.0 eV) and at a scattering angle of 90° . Based on the vibrational populations and the principle of detailed balance, these excitation functions are decomposed into contributions from state-to-state vibrational transitions involving up to the second bending overtone (030) in the electronically ground state. Both the2 Π resonance for COS around 1.2 eV and the2 Πu resonance for CO2 around 3.8 eV are shifted to lower energies as the initial vibrational state is excited in the bending mode. The width of the resonance hump for COS changes only little as the molecule bends, whereas that of the overall boomerang resonance for CO2 becomes narrower. The angular distribution of the electrons resonantly scattered by hot COS and hot CO2 is also measured. The different shapes depending on the vibrational transitions and gas temperatures are discussed in terms of the symmetry of the vibrational wave functions.
UR - http://www.scopus.com/inward/record.url?scp=85007592390&partnerID=8YFLogxK
U2 - 10.1140/epjd/e2016-70085-9
DO - 10.1140/epjd/e2016-70085-9
M3 - Article
AN - SCOPUS:85007592390
SN - 1434-6060
VL - 70
JO - European Physical Journal D
JF - European Physical Journal D
IS - 5
M1 - 100
ER -