2019A&A...632A.106L


Query : 2019A&A...632A.106L

2019A&A...632A.106L - Astronomy and Astrophysics, volume 632A106-106 (2019/12-0)

Physical conditions in the gas phases of the giant H II region LMC-N 11. II. Origin of [C II] and fraction of CO-dark gas.

LEBOUTEILLER V., CORMIER D., MADDEN S.C., GALAMETZ M., HONY S., GALLIANO F., CHEVANCE M., LEE M.-Y., BRAINE J., POLLES F.L., REQUENA-TORRES M.A., INDEBETOUW R., HUGHES A. and ABEL N.

Abstract (from CDS):


Context. The ambiguous origin of the [CII] 158µm line in the interstellar medium complicates its use for diagnostics concerning the star-formation rate and physical conditions in photodissociation regions.
Aims. We investigate the origin of [CII] in order to measure the total molecular gas content, the fraction of CO-dark H2 gas, and how these parameters are impacted by environmental effects such as stellar feedback.
Methods. We observed the giant HII region N 11 in the Large Magellanic Cloud with SOFIA/GREAT. The [CII] line is resolved in velocity and compared to HI and CO, using a Bayesian approach to decompose the line profiles. A simple model accounting for collisions in the neutral atomic and molecular gas was used in order to derive the H2 column density traced by C+.
Results. The profile of [CII] most closely resembles that of CO, but the integrated [CII] line width lies between that of CO and that of HI. Using various methods, we find that [CII] mostly originates from the neutral gas. We show that [CII] mostly traces the CO-dark H2 gas but there is evidence of a weak contribution from neutral atomic gas preferentially in the faintest components (as opposed to components with low [CII]/CO or low CO column density). Most of the molecular gas is CO-dark. The CO-dark H2 gas, whose density is typically a few 100s cm–3 and thermal pressure in the range 103.5–5K/cm3, is not always in pressure equilibrium with the neutral atomic gas. The fraction of CO-dark H2 gas decreases with increasing CO column density, with a slope that seems to depend on the impinging radiation field from nearby massive stars. Finally we extend previous measurements of the photoelectric-effect heating efficiency, which we find is constant across regions probed with Herschel, with [CII] and [OI] being the main coolants in faint and diffuse, and bright and compact regions, respectively, and with polycyclic aromatic hydrocarbon emission tracing the CO-dark H2 gas heating where [CII] and [OI] emit.
Conclusions. We present an innovative spectral decomposition method that allows statistical trends to be derived for the molecular gas content using CO, [CII], and HI profiles. Our study highlights the importance of velocity-resolved photodissociation region (PDR) diagnostics and higher spatial resolution for HI observations as future steps.

Abstract Copyright: © V. Lebouteiller et al. 2019

Journal keyword(s): ISM: general - photon-dominated region - Magellanic Clouds - submillimeter: ISM - infrared: ISM - galaxies: star formation

VizieR on-line data: <Available at CDS (J/A+A/632/A106): list.dat sp/*>

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 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
2 M 33 GiG 01 33 50.8965749232 +30 39 36.630403128 6.17 6.27 5.72     ~ 6226 1
3 NAME Magellanic Clouds GrG 03 00 -71.0           ~ 7988 0
4 LHA 120-N 11I HII 04 55 50 -66 34.4           ~ 19 0
5 LHA 120-N 11 HII 04 56 51.4 -66 24 24           ~ 275 0
6 NGC 1763 As* 04 56 51.5 -66 24 25     9.40     ~ 169 3
7 HD 32340 Em* 04 57 16.253 -66 23 20.94   13.11 12.45 14.00   O3-O6V 78 0
8 NGC 1769 As* 04 57 44.5 -66 27 42           ~ 73 1
9 LHA 120-N 11D EmO 04 57.8 -66 28           ~ 18 0
10 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
11 RMC 136 Cl* 05 38 42.396 -69 06 03.36   5.81 5.40     ~ 2236 2
12 LHA 120-N 159 HII 05 39 46.650 -69 45 39.94           ~ 293 2
13 NGC 4228 SBG 12 15 39.174 +36 19 36.80 10.63 10.30 9.93 9.74   ~ 1017 1
14 NAME M 17 SW SFR 18 20 23.1 -16 11 43           ~ 281 0

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