2015A&A...580A..83O


Query : 2015A&A...580A..83O

2015A&A...580A..83O - Astronomy and Astrophysics, volume 580A, 83-83 (2015/8-1)

Fine-structure line deficit in S 140.

OSSENKOPF V., KOUMPIA E., OKADA Y., MOOKERJEA B., VAN DER TAK F.F.S., SIMON R., PUETZ P. and GUESTEN R.

Abstract (from CDS):

We try to understand the gas heating and cooling in the S 140 star-forming region by spatially and spectrally resolving the distribution of the main cooling lines with GREAT/SOFIA and combining our data with existing ground-based and Herschel observations that trace the energy input and the density and temperature structure of the source. We mapped the fine-structure lines of [OI] (63µm) and [CII] (158µm) and the rotational transitions of CO 13-12 and 16-15 with GREAT/SOFIA and analyzed the spatial and velocity structure to assign the emission to individual heating sources. We measure the optical depth of the [CII] line and perform radiative transfer computations for all observed transitions. By comparing the line intensities with the far-infrared continuum we can assess the total cooling budget and measure the gas heating efficiency. The main emission of fine-structure lines in S 140 stems from a 8.3" region close to the infrared source IRS 2 that is not prominent at any other wavelength. It can be explained by a photon-dominated region (PDR) structure around the embedded cluster if we assume that the [Oi] line intensity is reduced by a factor of seven owing to self-absorption. The external cloud interface forms a second PDR at an inclination of 80-85 degrees illuminated by a UV field of 60 times the standard interstellar radiation field. The main radiation source in the cloud, IRS 1, is not prominent at all in the fine-structure lines. We measure line-to-continuum cooling ratios below 10–4, i.e. values lower than in any other Galactic source, actually matching the far-IR line deficit seen in ULIRGs. In particular, the low intensity of the [CII] line can only be modeled by an extreme excitation gradient in the gas around IRS 1. We found no explanation for why IRS 1 shows no associated fine-structure line peak, while IRS 2 does. The inner part of S 140 mimics the far-IR line deficit in ULIRGs thereby providing a template that may lead to a future model.

Abstract Copyright:

Journal keyword(s): ISM: individual objects: S 140 - ISM: structure - ISM: clouds - photon-dominated region (PDR) - ISM: abundances - ISM: lines and bands

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 - 2024
#notes
1 M 33 GiG 01 33 50.8965749232 +30 39 36.630403128 6.17 6.27 5.72     ~ 5839 1
2 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 17438 0
3 NGC 2024 Cl* 05 41 43 -01 50.5           ~ 1154 1
4 NAME Orion Molecular Cloud MoC 05 56 -01.8           ~ 1099 1
5 RAFGL 2046 HII 18 00 32.1 -24 04 03           ~ 362 0
6 W 49n HII 19 10 13.2 +09 06 12           ~ 470 3
7 HD 211880 EB* 22 18 27.8032795224 +63 13 22.448689068 7.47 7.99 7.75     B0.5V 102 0
8 SH 2-140 OpC 22 19 07.8 +63 17 07           ~ 658 2
9 NAME SH 2-140 IRS 1 Y*O 22 19 18.277 +63 18 45.82           ~ 197 0
10 NAME SH 2-140 IRS 2 NIR 22 19 18.514 +63 18 55.16           ~ 35 0
11 NAME SH 2-140 IRS 3 NIR 22 19 19.853 +63 18 48.07           ~ 47 0
12 LDN 1204 DNe 22 26.7 +63 15           ~ 87 1

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