2017MNRAS.471.1849D


Query : 2017MNRAS.471.1849D

2017MNRAS.471.1849D - Mon. Not. R. Astron. Soc., 471, 1849-1855 (2017/October-3)

Hyperfine excitation of C2H and C2D by para-H2.

DUMOUCHEL F., LIQUE F., SPIELFIEDEL A. and FEAUTRIER N.

Abstract (from CDS):

The [C2H]/[C2D] abundance ratio is a useful tool to explore the physical and chemical conditions of cold molecular clouds. Hence, an accurate determination of both the C2H and C2D abundances is of fundamental interest. Due to the low density of the interstellar medium, the population of the energy levels of the molecules is not at local thermodynamical equilibrium. Thus, the accurate modelling of the emission spectra requires the calculation of collisional rate coefficients with the most abundant interstellar species. Hence, we provide rate coefficients for the hyperfine excitation of C2H and C2D by para-H2(j=0), the most abundant collisional partner in cold molecular clouds. State-to-state rate coefficients between the lowest levels were computed for temperatures ranging from 5 to 80 K. For both isotopologues, the Δj = ΔF propensity rule is observed. The comparison between C2H and C2D rate coefficients shows that differences by up to a factor of two exist, mainly for Δj = ΔN = 1 transitions. The new rate coefficients will significantly help in the interpretation of recent observed spectra.

Abstract Copyright: © 2017 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society

Journal keyword(s): molecular data - molecular processes - scattering - scattering

Simbad objects: 6

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Number of rows : 6
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 TMC-1 MoC 04 41 45.9 +25 41 27           ~ 1872 0
2 NAME Orion-KL SFR 05 35 14.16 -05 22 21.5           ~ 2421 1
3 NAME Orion Bright Bar reg 05 35 22.30 -05 24 33.0           ~ 1004 0
4 NAME Ori A MoC 05 38 -07.1           ~ 3187 0
5 NAME Orion Molecular Cloud MoC 05 56 -01.8           ~ 1227 1
6 NAME Mon R2 HII 06 07 47.58 -06 22 42.6           ~ 789 2

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