Abstract

Context. The ambiguous origin of the [C II] 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 [C II] 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 H II region N 11 in the Large Magellanic Cloud with SOFIA/GREAT. The [C II] line is resolved in velocity and compared to H I 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 [C II] most closely resembles that of CO, but the integrated [C II] line width lies between that of CO and that of H I. Using various methods, we find that [C II] mostly originates from the neutral gas. We show that [C II] 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 [C II]/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 103.5−5 K cm−3, 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 [C II] and [O I] 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 [C II] and [O I] emit. Conclusions. We present an innovative spectral decomposition method that allows statistical trends to be derived for the molecular gas content using CO, [C II], and H I profiles. Our study highlights the importance of velocity-resolved photodissociation region (PDR) diagnostics and higher spatial resolution for H I observations as future steps.

Highlights

  • The [C II] 158 μm line emits under a variety of conditions in the interstellar medium (ISM) corresponding to the cold and warmThe reduced spectra are only available at the CDS via anonymous ftp to cdsarc.u-strasbg.fr (130.79.128.5) or via http://cdsarc. u-strasbg.fr/viz-bin/cat/J/A+A/632/A106 neutral medium and warm ionized gas, owing to the relatively low ionization potential to produce C+ ions (11.3 eV) and to the rtheleatniveeultyrallowgaesn, eCrg+ymoafytheex2iPst3/i2nfitnhee-sHtr0ucpthuareselebveult (91.3 K)

  • The remarkably small scatter in ([C II]+[O I])/polycyclic aromatic hydrocarbon (PAH) in many regions including photodissociation region (PDR) (#2) suggests that there is no significant extra [C II] emission arising from the ionized phase

  • The results agree with our study for Large Magellanic Cloud (LMC) data points, that is, bright [C II] components have a molecular gas fraction near unity, the contribution of neutral atomic gas to the [C II] emission is larger for faint [C II] components ( 6 × 10−8 W m−2 sr−1), and the fraction of CO-dark H2 gas decreases with the CO column density

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Summary

Introduction

The [C II] 158 μm line emits under a variety of conditions in the interstellar medium (ISM) corresponding to the cold and warmThe reduced spectra are only available at the CDS via anonymous ftp to cdsarc.u-strasbg.fr (130.79.128.5) or via http://cdsarc. u-strasbg.fr/viz-bin/cat/J/A+A/632/A106 neutral medium and warm ionized gas, owing to the relatively low ionization potential to produce C+ ions (11.3 eV) and to the rtheleatniveeultyrallowgaesn, eCrg+ymoafytheex2iPst3/i2nfitnhee-sHtr0ucpthuareselebveult (91.3 K). The spectral resolution in the optical tracers is not sufficient to decompose the velocity profiles but the fact that several velocity components may contribute to the observed ionized gas tracer profiles provides a useful constraint for the origin of [C II] based on its line width

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