2013MNRAS.431.3470H


Query : 2013MNRAS.431.3470H

2013MNRAS.431.3470H - Mon. Not. R. Astron. Soc., 431, 3470-3484 (2013/June-1)

Assessing molecular line diagnostics of triggered star formation using synthetic observations.

HAWORTH T.J., HARRIES T.J., ACREMAN D.M. and RUNDLE D.A.

Abstract (from CDS):

We investigate observational signatures of triggered star formation in bright rimmed clouds (BRCs) by using molecular line transfer calculations based on radiation-hydrodynamic radiatively driven implosion models. We find that for BRCs the separation in velocity between the line profile peak of an optically thick and an optically thin line is determined by both the observer viewing angle and the density of the shell driving into the cloud. In agreement with observations, we find that most BRC line profiles are symmetric and that asymmetries can be either red or blue, in contrast to the blue dominance expected for a collapsing cloud. Asymmetries in the line profiles arise when an optically thick line is dominated by the shell and an optically thin line is dominated by the cloud interior to the shell. The asymmetries are red or blue depending on whether the shell is moving towards or away from the observer, respectively. Using the known motions of the molecular gas in our models we rule out the `envelope expansion with core collapse' mechanism as the cause of the lack of blue-asymmetry in our simulated observations. We show that the absence of a strong photon-dominated region (PDR) around a BRC may not rule out the presence of triggered star formation: if the BRC line profile has a strong blue component then the shell is expected to be driving towards the observer, suggesting that the cloud is being viewed from behind and the PDR is obstructed. This could explain why BRCs such as SFO 80, 81 and 86 have a blue secondary peak and only a weak PDR inferred at 8µm. Finally we also test the use of 12CO, 13CO and C18O as diagnostics of cloud mass, temperature and column density. We find that the inferred conditions are in reasonable agreement with those from the models. Calculating the cloud mass assuming spherical symmetry is shown to introduce an error of an order of magnitude whereas integrating the column density over a given region is found to introduce an error of up to a factor of 2.

Abstract Copyright: © 2013 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2013)

Journal keyword(s): methods: numerical - methods: observational - stars: formation - ISM: clouds - H ii regions - ISM: kinematics and dynamics

Simbad objects: 14

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Number of rows : 14
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 IC 1848 OpC 02 51 19.4 +60 25 32   6.87 6.5     ~ 522 2
2 2MASX J02515372+6006564 MIR 02 51 53.730 +60 06 56.49           ~ 11 0
3 [KAG2008] globule 5 glb 02 51 53.91 +60 06 57.0           ~ 11 0
4 MSX6C G253.2934-01.6114 Cld 08 09 32.8 -36 05 00           ~ 11 0
5 MSX6C G260.7658+00.6604 Cld 08 41 13.0 -40 52 03           ~ 8 1
6 VdBH 26 RNe 08 58 04.3 -47 22 46 15.52 15.41 14.20     ~ 23 1
7 MSX6C G268.0574-00.9515 Cld 09 00 01.2 -47 31 37           ~ 5 1
8 IRAS 13050-6154 of? 13 08 12.15432 -62 10 22.8000           ~ 12 1
9 SFO 73 Cld 13 20 05.7 -62 24 03           ~ 6 1
10 IRAS 16362-4845 MoC 16 40 00.1 -48 51 45           ~ 20 2
11 MSX6C G336.6568-01.4099 Cld 16 40 16.8 -48 42 24           ~ 7 0
12 SFO 81 Cld 16 41 08.8 -49 17 45           ~ 5 0
13 SFO 86 Cld 17 49 36.1 -31 29 13           ~ 5 1
14 IRAS 17597-2422 Cld 18 02 51.6 -24 22 08           ~ 8 0

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