EXCITATION OF INTERSTELLAR HYDROGEN-CHLORIDE

Citation
Da. Neufeld et S. Green, EXCITATION OF INTERSTELLAR HYDROGEN-CHLORIDE, The Astrophysical journal, 432(1), 1994, pp. 158-166
Citations number
33
Categorie Soggetti
Astronomy & Astrophysics
Journal title
ISSN journal
0004637X
Volume
432
Issue
1
Year of publication
1994
Part
1
Pages
158 - 166
Database
ISI
SICI code
0004-637X(1994)432:1<158:EOIH>2.0.ZU;2-0
Abstract
We have computed new rate coefficients for the collisional excitation of HCI by He, in the close-coupled formalism and using an interaction potential determined recently by Willey, Choong, & DeLucia. Results ha ve been obtained for temperatures between 10 K and 300 K. With the use of the infinite order sudden approximation, we have derived approxima te expressions of general applicability which may be used to estimate how the rate constant for a transition (J --> J') is apportioned among the various hyperfine states F' of the final state J'. Using these ne w rate coefficients, we have obtained predictions for the HCI rotation al line strengths expected from a dense clump of interstellar gas, as a function of the HCI fractional abundance. Over a wide range of HCl a bundances, we have found that the line luminosities are proportional t o (abundance)2/3, a general result which can be explained using a simp le analytical approximation. Our model for the excitation of HCI withi n a dense molecular cloud core indicates that the J = 1-0 line strengt hs measured by Blake, Keene, & Phillips toward the Orion Molecular Clo ud (OMC-1) imply a fractional abundance n(HCl)/n(H-2) approximately 2 x 10(-9), a value which amounts to only approximately 0.3% of the cosm ic abundance of chlorine nuclei. Given a fractional abundance of 2 x 1 0(-9), the contribution of HCl emission to the total radiative cooling of a dense clump is small. For Orion, we predict a flux approximately 10(-19) W cm-2 for the HCl J = 3-2 line near 159.8 mum suggesting tha t the strength of this line could be measured using the Infrared Space Observatory.