2019MNRAS.489.4520N


Query : 2019MNRAS.489.4520N

2019MNRAS.489.4520N - Mon. Not. R. Astron. Soc., 489, 4520-4529 (2019/November-2)

C-type shock modelling - the effect of new H2-H collisional rate coefficients.

NESTERENOK A.V., BOSSION D., SCRIBANO Y. and LIQUE F.

Abstract (from CDS):

We consider collisional excitation of H2 molecules in C-type shocks propagating in dense molecular clouds. New data on collisional rate coefficients for (de-)excitation of H2 molecule in collisions with H atoms and new H2 dissociation rates are used. The new H2-H collisional data are state of the art and are based on the most accurate H3 potential energy surface. We re-examine the excitation of rotational levels of H2 molecule, the para-to-ortho-H2 conversion, and H2 dissociation by H2-H collisions. At cosmic ray ionization rates ζ >= 10–16 s–1 and at moderate shock speeds, the H/H2 ratio at the shock front is mainly determined by the cosmic ray ionization rate. The H2-H collisions play the main role in the para-to-ortho-H2 conversion and, at ζ >= 10–15 s–1, in the excitation of vibrationally excited states of H2 molecule in the shock. The H2ortho-to-para ratio of the shocked gas and column densities of rotational levels of vibrationally excited states of H2 are found to depend strongly on the cosmic ray ionization rate. We discuss the applicability of the presented results to interpretation of observations of H2 emission in supernova remnants.

Abstract Copyright: © 2019 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society

Journal keyword(s): molecular data - molecular processes - shock waves - ISM: supernova remnants

Simbad objects: 12

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Number of rows : 12
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 2MASS J03290842+3115284 NIR 03 29 08.420 +31 15 28.48           ~ 229 1
2 IC 443 SNR 06 17 00.0000000 +22 34 11.998901           ~ 1314 1
3 IC 443C PoC 06 17 44.2 +22 21 49           ~ 32 0
4 SNR G304.6+00.1 SNR 13 05 59 -62 42.0           ~ 93 0
5 SNR G346.6-00.2 SNR 17 10.3 -40 11           ~ 99 0
6 SNR G348.5-00.0 Rad 17 15 26 -38 28.0           ~ 39 1
7 SNR G349.7+00.2 SNR 17 18 10.160 -37 18 53.80           ~ 196 0
8 SNR G006.4-00.1 SNR 18 00 31.2011719 -23 25 48.001099           ~ 782 1
9 SNR G021.8-00.6 SNR 18 32 45 -10 08.0           ~ 137 0
10 SNR G031.9+00.0 SNR 18 49 16.3 -00 55 01           ~ 368 2
11 SNR G034.6-00.5 SNR 18 56 10.650 +01 13 21.30           ~ 1034 2
12 SNR G039.2-00.3 SNR 19 04 03.9 +05 26 56           ~ 204 1

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