2012A&A...543A.145P


Query : 2012A&A...543A.145P

2012A&A...543A.145P - Astronomy and Astrophysics, volume 543A145-145 (2012/7-1)

Nitrogen hydrides in interstellar gas. II. Analysis of Herschel/HIFI observations towards W49N and G10.6-0.4 (W31C).

PERSSON C.M., DE LUCA M., MOOKERJEA B., OLOFSSON A.O.H., BLACK J.H., GERIN M., HERBST E., BELL T.A., COUTENS A., GODARD B., GOICOECHEA J.R., HASSEL G.E., HILY-BLANT P., MENTEN K.M., MUELLER H.S.P., PEARSON J.C. and YU S.

Abstract (from CDS):

As a part of the Herschel key programme PRISMAS, we have used the Herschel/HIFI instrument to observe interstellar nitrogen hydrides along the sight-lines towards eight high-mass star-forming regions in order to elucidate the production pathways leading to nitrogen-bearing species in diffuse gas. Here, we report observations towards W49N of the NH N=1-0, J=2-1, and J=1-0, ortho-NH2 NKa_, KcJ=11,13/2–00,0_1/2, ortho-NH3 JK=10-00 and 20-10, para-NH3 JK=21-11 transitions, and unsuccessful searches for NH+. All detections show absorption by foreground material over a wide range of velocities, as well as absorption associated directly with the hot-core source itself. As in the previously published observations towards G10.6-0.4, the NH, NH2 and NH3 spectra towards W49N show strikingly similar and non-saturated absorption features. We decompose the absorption of the foreground material towards W49N into different velocity components in order to investigate whether the relative abundances vary among the velocity components, and, in addition, we re-analyse the absorption lines towards G10.6-0.4 in the same manner. Abundances, with respect to molecular hydrogen, in each velocity component are estimated using CH, which is found to correlate with H2 in the solar neighbourhood diffuse gas. The analysis points to a co-existence of the nitrogen hydrides in diffuse or translucent interstellar gas with a high molecular fraction. Towards both sources, we find that NH is always at least as abundant as both o-NH2 and o-NH3, in sharp contrast to previous results for dark clouds. We find relatively constant N(NH)/N(o-NH3) and N(o-NH2)/N(o-NH3) ratios with mean values of 3.2 and 1.9 towards W49N, and 5.4 and 2.2 towards G10.6-0.4, respectively. The mean abundance of o-NH3 is ∼2x10–9 towards both sources. The nitrogen hydrides also show linear correlations with CN and HNC towards both sources, and looser correlations with CH. The upper limits on the NH+ abundance indicate column densities ≲2-14% of N(NH), which is in contrast to the behaviour of the abundances of CH+ and OH+ relative to the values determined for the corresponding neutrals CH and OH. Surprisingly low values of the ammonia ortho-to-para ratio are found in both sources, ≃0.5-0.7±0.1, in the strongest absorption components. This result cannot be explained by current models as we had expected to find a value of unity or higher.

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Journal keyword(s): astrochemistry - line: formation - ISM: abundances - ISM: molecules - submillimeter: ISM - molecular processes

Simbad objects: 16

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Number of rows : 16
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 NAME Orion-KL SFR 05 35 14.16 -05 22 21.5           ~ 2421 1
2 HD 124314 ** 14 15 01.60615 -61 42 24.3831   8.96 6.64 6.45 6.31 O6V(n)((f)) 155 0
3 * rho Oph ** 16 25 35.11766 -23 26 49.8150 4.30 4.85 4.63 4.27 3.96 B2IV+B2V 670 0
4 IRAS 16293-2422 cor 16 32 22.56 -24 28 31.8           ~ 1357 1
5 NAME Galactic Center reg 17 45 39.60213 -29 00 22.0000           ~ 16269 0
6 NAME Sgr A* X 17 45 40.03599 -29 00 28.1699           ~ 4970 3
7 NAME Sgr B2 MoC 17 47 20.4 -28 23 07           ~ 2443 1
8 W 28a Rad 18 00 30.4 -24 03 58           ~ 31 0
9 W 31 SFR 18 10 28.6 -19 55 51           ~ 280 0
10 W 31c HII 18 10 29.1 -19 56 05           ~ 357 0
11 W 33a Y*O 18 14 39.56547 -17 52 02.2260           ~ 746 0
12 GAL 034.3+00.1 SFR 18 53 22 +01 14.6           ~ 31 0
13 W 49n HII 19 10 13.2 +09 06 12           ~ 497 3
14 W 51 SNR 19 23 50 +14 06.0           ~ 1352 1
15 DR 21 (OH) cor 20 39 01.01 +42 22 50.2           ~ 427 0
16 LDN 1157 DNe 20 39 06.4 +68 02 13           ~ 606 0

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