2022
DOI: 10.1063/1674-0068/cjcp2112271
|View full text |Cite
|
Sign up to set email alerts
|

Vacuum ultraviolet photodissociation dynamics of OCS via the F Rydberg state: The S(3PJ = 2, 1, 0) product channels

Abstract: Vacuum ultraviolet (VUV) photodissociation dynamics of carbonyl sulfide was investigated experimentally by using a tunable photolysis light source and the time-sliced velocity map ion imaging technique. Ion images of S(3P J =2, 1, 0) dissociation products were measured at five photolysis wavelengths from 133.26 nm to 139.96 nm, corresponding to the F Rydberg state of OCS. Two dissociation channels: S(3P J)+CO( X1Σ+) and S(3P J)+CO( A3Π) were observed with the former being dominant. The vibrational states of CO… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2

Citation Types

0
2
0

Year Published

2023
2023
2024
2024

Publication Types

Select...
4

Relationship

2
2

Authors

Journals

citations
Cited by 4 publications
(2 citation statements)
references
References 47 publications
0
2
0
Order By: Relevance
“…The product total translational energy, P ( E T ), distributions were obtained using tunable VUV pump and probe sources along with HRTOF detection . The experimental apparatus and methods have been detailed previously. , The H 2 S sample (typically 30% seeded in Ar) was introduced into the interaction volume in the form of a pulsed jet. The photolysis photons at λ ∼ 129.1 nm were generated by difference four-wave mixing (DFWM) involving two λ = 212.556 nm photons, and one λ ∼ 600 nm photon overlapped in a stainless-steel cell filled with a 3:1 ratio Ar/Kr gas mixture.…”
Section: Experimental Methodsmentioning
confidence: 99%
“…The product total translational energy, P ( E T ), distributions were obtained using tunable VUV pump and probe sources along with HRTOF detection . The experimental apparatus and methods have been detailed previously. , The H 2 S sample (typically 30% seeded in Ar) was introduced into the interaction volume in the form of a pulsed jet. The photolysis photons at λ ∼ 129.1 nm were generated by difference four-wave mixing (DFWM) involving two λ = 212.556 nm photons, and one λ ∼ 600 nm photon overlapped in a stainless-steel cell filled with a 3:1 ratio Ar/Kr gas mixture.…”
Section: Experimental Methodsmentioning
confidence: 99%
“…The photodissociation of OCS at near UV wavelengths λ >200 nm is dominated by the spin-allowed channel yielding S( 1 D) + CO(X) products; the latter are formed vibrationally ‘cold’ but rotationally ‘hot’, in at least qualitative accord with that expected given the forces introduced by a bent ← linear excitation process [ 84 ]. The same product channel has been investigated using TSVMI methods following excitation in the range 142.98 ≤ λ ≤ 154.37 nm [ 75 ] and other single-bond fission channels yielding S( 1 S) + CO(X) [ 85 ] and S( 3 P) + CO(A) [ 86 ] products have also been reported when exciting at similar VUV wavelengths.…”
Section: Experimental Methodsmentioning
confidence: 99%